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overflow: hidden; text-overflow: ellipsis; -webkit-line-clamp: 3; -webkit-box-orient: vertical; }</style><div class="col-xs-12 clearfix"><div class="u-floatLeft"><h1 class="PageHeader-title u-m0x u-fs30">HIGH TEMPERATURE SUPERCONDUCTIVITY</h1><div class="u-tcGrayDark">9,909 Followers</div><div class="u-tcGrayDark u-mt2x">Recent papers in <b>HIGH TEMPERATURE SUPERCONDUCTIVITY</b></div></div></div></div></div></div><div class="TabbedNavigation"><div class="container"><div class="row"><div class="col-xs-12 clearfix"><ul class="nav u-m0x u-p0x list-inline u-displayFlex"><li class="active"><a href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">Top Papers</a></li><li><a href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY/MostCited">Most Cited Papers</a></li><li><a href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY/MostDownloaded">Most Downloaded Papers</a></li><li><a href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY/MostRecent">Newest Papers</a></li><li><a class="" href="https://www.academia.edu/People/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">People</a></li></ul></div><style type="text/css">ul.nav{flex-direction:row}@media(max-width: 567px){ul.nav{flex-direction:column}.TabbedNavigation li{max-width:100%}.TabbedNavigation li.active{background-color:var(--background-grey, #dddde2)}.TabbedNavigation li.active:before,.TabbedNavigation li.active:after{display:none}}</style></div></div></div><div class="container"><div class="row"><div class="col-xs-12"><div class="u-displayFlex"><div class="u-flexGrow1"><div class="works"><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_11837429" data-work_id="11837429" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/11837429/Experiences_Determining_the_AC_Current_Rating_of_HTS_Tapes_in_Power_Transformers">Experiences Determining the AC Current Rating of HTS Tapes in Power Transformers</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Two experimental high temperature superconducting transformers has been designed and built using Bi2223 HTS tape. The transformers are unique in that the magnetic circuit is comprised of air and a silicon steel partial core. The first... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_11837429" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Two experimental high temperature superconducting transformers has been designed and built using Bi2223 HTS tape. The transformers are unique in that the magnetic circuit is comprised of air and a silicon steel partial core. The first transformer failed during a full load endurance run and an investigation was carried out to determine the cause of the failure. The cause was believed to be from operating the HTS windings close to critical conditions. A method of determining the ac current rating of the HTS tape was developed and applied to the second transformer. This second transformer was tested successfully under load for several hours.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/11837429" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="265a5d4d1694b278b54d713f55440250" rel="nofollow" data-download="{"attachment_id":37238093,"asset_id":11837429,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/37238093/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="18009526" href="https://canterbury-nz.academia.edu/AndrewLapthorn">Andrew Lapthorn</a><script data-card-contents-for-user="18009526" type="text/json">{"id":18009526,"first_name":"Andrew","last_name":"Lapthorn","domain_name":"canterbury-nz","page_name":"AndrewLapthorn","display_name":"Andrew Lapthorn","profile_url":"https://canterbury-nz.academia.edu/AndrewLapthorn?f_ri=34232","photo":"https://0.academia-photos.com/18009526/11854660/13211922/s65_andrew.lapthorn.jpg"}</script></span></span></li><li class="js-paper-rank-work_11837429 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="11837429"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 11837429, container: ".js-paper-rank-work_11837429", }); 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$(".js-view-count[data-work-id=11837429]").text(description); $(".js-view-count-work_11837429").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_11837429").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="11837429"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">2</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a>, <script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="199698" rel="nofollow" href="https://www.academia.edu/Documents/in/Power_transformers">Power transformers</a><script data-card-contents-for-ri="199698" type="text/json">{"id":199698,"name":"Power transformers","url":"https://www.academia.edu/Documents/in/Power_transformers?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=11837429]'), work: {"id":11837429,"title":"Experiences Determining the AC Current Rating of HTS Tapes in Power Transformers","created_at":"2015-04-07T17:35:08.679-07:00","url":"https://www.academia.edu/11837429/Experiences_Determining_the_AC_Current_Rating_of_HTS_Tapes_in_Power_Transformers?f_ri=34232","dom_id":"work_11837429","summary":"Two experimental high temperature superconducting transformers has been designed and built using Bi2223 HTS tape. The transformers are unique in that the magnetic circuit is comprised of air and a silicon steel partial core. The first transformer failed during a full load endurance run and an investigation was carried out to determine the cause of the failure. The cause was believed to be from operating the HTS windings close to critical conditions. A method of determining the ac current rating of the HTS tape was developed and applied to the second transformer. This second transformer was tested successfully under load for several hours.","downloadable_attachments":[{"id":37238093,"asset_id":11837429,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":18009526,"first_name":"Andrew","last_name":"Lapthorn","domain_name":"canterbury-nz","page_name":"AndrewLapthorn","display_name":"Andrew Lapthorn","profile_url":"https://canterbury-nz.academia.edu/AndrewLapthorn?f_ri=34232","photo":"https://0.academia-photos.com/18009526/11854660/13211922/s65_andrew.lapthorn.jpg"}],"research_interests":[{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":199698,"name":"Power transformers","url":"https://www.academia.edu/Documents/in/Power_transformers?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_7978295" data-work_id="7978295" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/7978295/Effect_of_activation_temperature_on_pore_development_in_activated_carbon_produced_from_palm_cell">Effect of activation temperature on pore development in activated carbon produced from palm cell</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">A series of experiments were conducted to investigate the effect of activation temperature on pore development of activated carbon produced from palm shell. Activation of the samples was carried out at 800, 850 and 900°C for different... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_7978295" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">A series of experiments were conducted to investigate the effect of activation temperature on pore development of activated carbon produced from palm shell. Activation of the samples was carried out at 800, 850 and 900°C for different durations ranging from 10 to 180min. The samples were characterized using N2 adsorption for evaluation of micropores and the mercury intrusion technique for mesopore and macropore analysis. Within the range of activation temperatures studied, high burn-off products derived from high activation temperatures tend to have larger micropore development. However, an increase in the activation temperature has no remarkable effect on mesopore and macropore development. © 2002 Society of Chemical Industry. <br /> <br /><a href="http://onlinelibrary.wiley.com/store/10.1002/jctb.712/asset/712_ftp.pdf?v=1&t=hytj8q2o&s=714078f9999ade816b5eb3df8f7774e5c13db2b5" rel="nofollow">http://onlinelibrary.wiley.com/store/10.1002/jctb.712/asset/712_ftp.pdf?v=1&t=hytj8q2o&s=714078f9999ade816b5eb3df8f7774e5c13db2b5</a></div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/7978295" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="6a59feed4bee3e16b8dbbe890f75e098" rel="nofollow" data-download="{"attachment_id":34447138,"asset_id":7978295,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/34447138/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="15105238" href="https://malaya.academia.edu/WanMohdAshriWanDaud">Wan Mohd Ashri Wan Daud</a><script data-card-contents-for-user="15105238" type="text/json">{"id":15105238,"first_name":"Wan Mohd Ashri","last_name":"Wan Daud","domain_name":"malaya","page_name":"WanMohdAshriWanDaud","display_name":"Wan Mohd Ashri Wan Daud","profile_url":"https://malaya.academia.edu/WanMohdAshriWanDaud?f_ri=34232","photo":"https://0.academia-photos.com/15105238/4222326/4914483/s65_wan_mohd_ashri.wan_daud.jpg"}</script></span></span></li><li class="js-paper-rank-work_7978295 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="7978295"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 7978295, container: ".js-paper-rank-work_7978295", }); 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Activation of the samples was carried out at 800, 850 and 900°C for different durations ranging from 10 to 180min. The samples were characterized using N2 adsorption for evaluation of micropores and the mercury intrusion technique for mesopore and macropore analysis. Within the range of activation temperatures studied, high burn-off products derived from high activation temperatures tend to have larger micropore development. However, an increase in the activation temperature has no remarkable effect on mesopore and macropore development. © 2002 Society of Chemical Industry.\r\n\r\nhttp://onlinelibrary.wiley.com/store/10.1002/jctb.712/asset/712_ftp.pdf?v=1\u0026t=hytj8q2o\u0026s=714078f9999ade816b5eb3df8f7774e5c13db2b5 ","downloadable_attachments":[{"id":34447138,"asset_id":7978295,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":15105238,"first_name":"Wan Mohd Ashri","last_name":"Wan Daud","domain_name":"malaya","page_name":"WanMohdAshriWanDaud","display_name":"Wan Mohd Ashri Wan Daud","profile_url":"https://malaya.academia.edu/WanMohdAshriWanDaud?f_ri=34232","photo":"https://0.academia-photos.com/15105238/4222326/4914483/s65_wan_mohd_ashri.wan_daud.jpg"}],"research_interests":[{"id":395,"name":"Experimental Archaeology","url":"https://www.academia.edu/Documents/in/Experimental_Archaeology?f_ri=34232","nofollow":true},{"id":14989,"name":"Philosophy of Time","url":"https://www.academia.edu/Documents/in/Philosophy_of_Time?f_ri=34232","nofollow":true},{"id":31893,"name":"Industrial wastewater Treatment","url":"https://www.academia.edu/Documents/in/Industrial_wastewater_Treatment?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":43307,"name":"Oil Industry","url":"https://www.academia.edu/Documents/in/Oil_Industry?f_ri=34232"},{"id":62537,"name":"Porosity and Permeability in Reservoirs","url":"https://www.academia.edu/Documents/in/Porosity_and_Permeability_in_Reservoirs?f_ri=34232"},{"id":77006,"name":"CHEMICAL REACTION ENGINEERING-OCTAVE LEVENSPIEL","url":"https://www.academia.edu/Documents/in/CHEMICAL_REACTION_ENGINEERING-OCTAVE_LEVENSPIEL?f_ri=34232"},{"id":113095,"name":"Adsorption and wastewater treatment","url":"https://www.academia.edu/Documents/in/Adsorption_and_wastewater_treatment?f_ri=34232"},{"id":133177,"name":"Temperature","url":"https://www.academia.edu/Documents/in/Temperature?f_ri=34232"},{"id":139774,"name":"Biological Nitrogen Fixation","url":"https://www.academia.edu/Documents/in/Biological_Nitrogen_Fixation?f_ri=34232"},{"id":168891,"name":"Chemical Analysis","url":"https://www.academia.edu/Documents/in/Chemical_Analysis?f_ri=34232"},{"id":169415,"name":"Article","url":"https://www.academia.edu/Documents/in/Article?f_ri=34232"},{"id":172270,"name":"Neutron Activation Analysis","url":"https://www.academia.edu/Documents/in/Neutron_Activation_Analysis?f_ri=34232"},{"id":173897,"name":"Mesoporous Materials","url":"https://www.academia.edu/Documents/in/Mesoporous_Materials?f_ri=34232"},{"id":425968,"name":"Independent-Sample T-Test","url":"https://www.academia.edu/Documents/in/Independent-Sample_T-Test?f_ri=34232"},{"id":466389,"name":"Palm Shell","url":"https://www.academia.edu/Documents/in/Palm_Shell?f_ri=34232"},{"id":546352,"name":"Controlled Study","url":"https://www.academia.edu/Documents/in/Controlled_Study?f_ri=34232"},{"id":1175972,"name":"Assessing the Effectiveness of Waste Water Treatment Plants In the Removal of Heavy Metal Mercury and Lead","url":"https://www.academia.edu/Documents/in/Assessing_the_Effectiveness_of_Waste_Water_Treatment_Plants_In_the_Removal_of_Heavy_Metal_Mercury_an?f_ri=34232"},{"id":1491507,"name":"Pore development","url":"https://www.academia.edu/Documents/in/Pore_development?f_ri=34232"},{"id":1491563,"name":"Activation temperature","url":"https://www.academia.edu/Documents/in/Activation_temperature?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_28783836" data-work_id="28783836" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/28783836/The_BCS_theory_of_superconductivity_revisited_quasiparticle_imbalance_in_equilibrium_and_multiple_solutions_of_the_energy_gap_equation">The BCS theory of superconductivity revisited: quasiparticle imbalance in equilibrium and multiple solutions of the energy gap equation</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">We examine the equilibrium solutions of the BCS theory of superconductivity in the low temperature limit, allowing the attraction band to be asymmetric with respect to the chemical potential of the system µR. If we denote by µ the middle... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_28783836" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">We examine the equilibrium solutions of the BCS theory of superconductivity in the low temperature limit, allowing the attraction band to be asymmetric with respect to the chemical potential of the system µR. If we denote by µ the middle of the attraction band, we observe that the super-conducting phase is formed only if |µR − µ| < 2∆0, where ∆0 is the energy gap at zero temperature in the standard BCS theory. If |µR − µ| < 2∆0, the system of equations which give the energy gap has two solutions for each value of µR − µ: one with ∆(T = 0) = ∆0 and another one, with ∆(T = 0) < ∆0 (∆(T = 0) is the energy gap at 0 K). If 0 < |µR − µ| < 2∆0, a quasiparticle imbalance appears in equilibrium. In the " standard BCS limit, " which is µR → µ, beside the standard solution ∆(T = 0) = ∆0, we find another one, with ∆(T = 0) = ∆0/3 and nonzero quasiparticle population. The formalism takes into account in a consistent way the variation of the total number of particles with the population of the quasiparticle states.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/28783836" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="7ffce2bdef9561ff2e2a8d797e1b17d7" rel="nofollow" data-download="{"attachment_id":49202832,"asset_id":28783836,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/49202832/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="22327263" href="https://ifin.academia.edu/DragosAnghel">Dragos-Victor Anghel</a><script data-card-contents-for-user="22327263" type="text/json">{"id":22327263,"first_name":"Dragos-Victor","last_name":"Anghel","domain_name":"ifin","page_name":"DragosAnghel","display_name":"Dragos-Victor Anghel","profile_url":"https://ifin.academia.edu/DragosAnghel?f_ri=34232","photo":"https://0.academia-photos.com/22327263/6103244/21226686/s65_dragos-victor.anghel.jpg"}</script></span></span></li><li class="js-paper-rank-work_28783836 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="28783836"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 28783836, container: ".js-paper-rank-work_28783836", }); 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If we denote by µ the middle of the attraction band, we observe that the super-conducting phase is formed only if |µR − µ| \u003c 2∆0, where ∆0 is the energy gap at zero temperature in the standard BCS theory. If |µR − µ| \u003c 2∆0, the system of equations which give the energy gap has two solutions for each value of µR − µ: one with ∆(T = 0) = ∆0 and another one, with ∆(T = 0) \u003c ∆0 (∆(T = 0) is the energy gap at 0 K). If 0 \u003c |µR − µ| \u003c 2∆0, a quasiparticle imbalance appears in equilibrium. In the \" standard BCS limit, \" which is µR → µ, beside the standard solution ∆(T = 0) = ∆0, we find another one, with ∆(T = 0) = ∆0/3 and nonzero quasiparticle population. The formalism takes into account in a consistent way the variation of the total number of particles with the population of the quasiparticle states.","downloadable_attachments":[{"id":49202832,"asset_id":28783836,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":22327263,"first_name":"Dragos-Victor","last_name":"Anghel","domain_name":"ifin","page_name":"DragosAnghel","display_name":"Dragos-Victor Anghel","profile_url":"https://ifin.academia.edu/DragosAnghel?f_ri=34232","photo":"https://0.academia-photos.com/22327263/6103244/21226686/s65_dragos-victor.anghel.jpg"}],"research_interests":[{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":277776,"name":"Quantum and classical statistical 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js-work-link" rel="nofollow" href="https://www.academia.edu/8212849/Low_Power_Starship_Warp_Drive_Excerpt_from_Stardrive_book_090514_">Low Power Starship Warp Drive (Excerpt from Stardrive book 090514)</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">A smart high Tc superconductor meta-material with off mass-shell near field resonances is predicted to behave like the exotic matter needed for weightless geodesic warp drive as well as for the wormhole time machines depicted in Kip... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_8212849" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">A smart high Tc superconductor meta-material with off mass-shell near field resonances is predicted to behave like the exotic matter needed for weightless geodesic warp drive as well as for the wormhole time machines 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metamaterials","url":"https://www.academia.edu/Documents/in/Electromagnetic_metamaterials?f_ri=34232","nofollow":true},{"id":10018,"name":"Metamaterials","url":"https://www.academia.edu/Documents/in/Metamaterials?f_ri=34232"},{"id":11541,"name":"Graphene","url":"https://www.academia.edu/Documents/in/Graphene?f_ri=34232"},{"id":11973,"name":"Nanomaterials","url":"https://www.academia.edu/Documents/in/Nanomaterials?f_ri=34232"},{"id":17733,"name":"Nanotechnology","url":"https://www.academia.edu/Documents/in/Nanotechnology?f_ri=34232"},{"id":31371,"name":"Time Travel","url":"https://www.academia.edu/Documents/in/Time_Travel?f_ri=34232"},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232"},{"id":103213,"name":"Nanoscience","url":"https://www.academia.edu/Documents/in/Nanoscience?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_4092484" data-work_id="4092484" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/4092484/A_technical_note_on_the_production_of_zirconia_and_zircon_brick_from_locally_available_zircon_in_Bangladesh">A technical note on the production of zirconia and zircon brick from locally available zircon in Bangladesh</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">In this study, the potentiality of Bangladesh zircon as a raw material for zirconia and zircon brick production was examined. Decomposition of zircon (ZrSiO4) into zirconia (ZrO2) was attempted by using caustic soda (NaOH) as the... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_4092484" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">In this study, the potentiality of Bangladesh zircon as a raw material for zirconia and zircon brick production was examined. Decomposition of zircon (ZrSiO4) into zirconia (ZrO2) was attempted by using caustic soda (NaOH) as the decomposition agent. 5-10 μm size zircon, 5-30 wt.% NaOH, and decomposition temperatures ranging from 1300 to 1500°C were investigated. X-ray diffraction method using Mo Kα radiation was used in order to find out the extent of decomposition of zircon into zirconia. Zircon bricks of 0.06 mm× 0.06 mm× 0.025 mm shaped were made under a pressure of 15 MPa. Carboxi methyal cellulose (CMC) and Fe2O 3 were used as a binder. With increasing temperature and percentage of NaOH, decomposition of zircon increases. Crushing strengths and density of these bricks could be found as high as 53.36 MPa and 3210 kg/m3, respectively. Bangladesh zircon can be used successfully for preparation of refractory bricks for high temperature use. <br /> <br /><a href="http://www.sciencedirect.com/science/article/pii/S092401360500909X" rel="nofollow">http://www.sciencedirect.com/science/article/pii/S092401360500909X</a></div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/4092484" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="3d6cbe9cb7479c2dcf6a51827505b077" rel="nofollow" data-download="{"attachment_id":31616635,"asset_id":4092484,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/31616635/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="3054445" href="https://malaya.academia.edu/HaseebASMA">Haseeb ASMA</a><script data-card-contents-for-user="3054445" type="text/json">{"id":3054445,"first_name":"Haseeb","last_name":"ASMA","domain_name":"malaya","page_name":"HaseebASMA","display_name":"Haseeb ASMA","profile_url":"https://malaya.academia.edu/HaseebASMA?f_ri=34232","photo":"https://0.academia-photos.com/3054445/1004285/1255894/s65_haseeb.asma.jpg"}</script></span></span></li><li class="js-paper-rank-work_4092484 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="4092484"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 4092484, container: ".js-paper-rank-work_4092484", }); 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$(".js-view-count[data-work-id=4092484]").text(description); $(".js-view-count-work_4092484").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_4092484").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="4092484"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">15</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="6414" rel="nofollow" href="https://www.academia.edu/Documents/in/Decomposition">Decomposition</a>, <script data-card-contents-for-ri="6414" type="text/json">{"id":6414,"name":"Decomposition","url":"https://www.academia.edu/Documents/in/Decomposition?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="17395" rel="nofollow" href="https://www.academia.edu/Documents/in/Density-functional_theory">Density-functional theory</a>, <script data-card-contents-for-ri="17395" type="text/json">{"id":17395,"name":"Density-functional theory","url":"https://www.academia.edu/Documents/in/Density-functional_theory?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="21598" rel="nofollow" href="https://www.academia.edu/Documents/in/Brick_and_tile_Archaeology_">Brick and tile (Archaeology)</a>, <script data-card-contents-for-ri="21598" type="text/json">{"id":21598,"name":"Brick and tile (Archaeology)","url":"https://www.academia.edu/Documents/in/Brick_and_tile_Archaeology_?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=4092484]'), work: {"id":4092484,"title":"A technical note on the production of zirconia and zircon brick from locally available zircon in Bangladesh","created_at":"2013-07-23T17:32:39.364-07:00","url":"https://www.academia.edu/4092484/A_technical_note_on_the_production_of_zirconia_and_zircon_brick_from_locally_available_zircon_in_Bangladesh?f_ri=34232","dom_id":"work_4092484","summary":"In this study, the potentiality of Bangladesh zircon as a raw material for zirconia and zircon brick production was examined. Decomposition of zircon (ZrSiO4) into zirconia (ZrO2) was attempted by using caustic soda (NaOH) as the decomposition agent. 5-10 μm size zircon, 5-30 wt.% NaOH, and decomposition temperatures ranging from 1300 to 1500°C were investigated. X-ray diffraction method using Mo Kα radiation was used in order to find out the extent of decomposition of zircon into zirconia. Zircon bricks of 0.06 mm× 0.06 mm× 0.025 mm shaped were made under a pressure of 15 MPa. Carboxi methyal cellulose (CMC) and Fe2O 3 were used as a binder. With increasing temperature and percentage of NaOH, decomposition of zircon increases. Crushing strengths and density of these bricks could be found as high as 53.36 MPa and 3210 kg/m3, respectively. Bangladesh zircon can be used successfully for preparation of refractory bricks for high temperature use. \r\n\r\nhttp://www.sciencedirect.com/science/article/pii/S092401360500909X ","downloadable_attachments":[{"id":31616635,"asset_id":4092484,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":3054445,"first_name":"Haseeb","last_name":"ASMA","domain_name":"malaya","page_name":"HaseebASMA","display_name":"Haseeb ASMA","profile_url":"https://malaya.academia.edu/HaseebASMA?f_ri=34232","photo":"https://0.academia-photos.com/3054445/1004285/1255894/s65_haseeb.asma.jpg"}],"research_interests":[{"id":6414,"name":"Decomposition","url":"https://www.academia.edu/Documents/in/Decomposition?f_ri=34232","nofollow":true},{"id":17395,"name":"Density-functional theory","url":"https://www.academia.edu/Documents/in/Density-functional_theory?f_ri=34232","nofollow":true},{"id":21598,"name":"Brick and tile (Archaeology)","url":"https://www.academia.edu/Documents/in/Brick_and_tile_Archaeology_?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":60658,"name":"Numerical Simulation","url":"https://www.academia.edu/Documents/in/Numerical_Simulation?f_ri=34232"},{"id":133177,"name":"Temperature","url":"https://www.academia.edu/Documents/in/Temperature?f_ri=34232"},{"id":206457,"name":"Zircon","url":"https://www.academia.edu/Documents/in/Zircon?f_ri=34232"},{"id":218344,"name":"Effects of Temperature on the Compressive Strength of a Concrete","url":"https://www.academia.edu/Documents/in/Effects_of_Temperature_on_the_Compressive_Strength_of_a_Concrete?f_ri=34232"},{"id":314122,"name":"Physicochemical Properties of Clay in Refractory Bricks Physics","url":"https://www.academia.edu/Documents/in/Physicochemical_Properties_of_Clay_in_Refractory_Bricks_Physics?f_ri=34232"},{"id":340662,"name":"Zirconia","url":"https://www.academia.edu/Documents/in/Zirconia?f_ri=34232"},{"id":902446,"name":"X Ray Diffraction Analysis","url":"https://www.academia.edu/Documents/in/X_Ray_Diffraction_Analysis?f_ri=34232"},{"id":908283,"name":"Crushing Strength","url":"https://www.academia.edu/Documents/in/Crushing_Strength?f_ri=34232"},{"id":908284,"name":"NaOH","url":"https://www.academia.edu/Documents/in/NaOH?f_ri=34232"},{"id":963945,"name":"Focal Laser Ablation","url":"https://www.academia.edu/Documents/in/Focal_Laser_Ablation?f_ri=34232"},{"id":963950,"name":"Damage Distribution","url":"https://www.academia.edu/Documents/in/Damage_Distribution?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_38537495" data-work_id="38537495" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/38537495/ROBOTIC_CAR_USING_ARDUINO_WITH_BLUETOOTH_CONTROLLER">ROBOTIC CAR USING ARDUINO WITH BLUETOOTH CONTROLLER</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">The Android controlled temperature sensing RoboCar. The working is based on Android OS, Arduino, L298N motor, DC motor driver, temperature sensor-DHT11 and Bluetooth module. Arduino is an open-source prototype platform. Sensing the... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_38537495" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">The Android controlled temperature sensing RoboCar. The working is based on Android OS, Arduino, L298N motor, DC motor driver, temperature sensor-DHT11 and Bluetooth module. Arduino is an open-source prototype platform. Sensing the environment of the temperature sensor. Remote control car, with an Arduino, L298N motor and Bluetooth module. Sensing the temperature, with an DHT11, Arduino and Bluetooth module. Upload the code to the Arduino using the knowledge of programming. The Arduino code simulated on software and be interface with the hardware. The device can be controlled by any smart device with android. AirDroid is an app exclusive to Android which enables you to connect your device to PC through a Wi-Fi controller of wireless network. It is used to connect the mobile camera to view in our pc to fixing in the car. It also used to view the location of the car. The Robotic car sense the temperature to view by the mobile app. All the controls of the vehicle on the app on that device. It is used to sense the environment of the military force before doing some of the process. It is used for the sensing the environment of the system.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/38537495" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="9a8d5df033b61c00a6c3d899ea129254" rel="nofollow" data-download="{"attachment_id":58607857,"asset_id":38537495,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/58607857/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="104799352" href="https://independent.academia.edu/SushiSushi1">Vijayalakshmi Selvaraj</a><script data-card-contents-for-user="104799352" type="text/json">{"id":104799352,"first_name":"Vijayalakshmi","last_name":"Selvaraj","domain_name":"independent","page_name":"SushiSushi1","display_name":"Vijayalakshmi Selvaraj","profile_url":"https://independent.academia.edu/SushiSushi1?f_ri=34232","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_38537495 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="38537495"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 38537495, container: ".js-paper-rank-work_38537495", }); 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The working is based on Android OS, Arduino, L298N motor, DC motor driver, temperature sensor-DHT11 and Bluetooth module. Arduino is an open-source prototype platform. Sensing the environment of the temperature sensor. Remote control car, with an Arduino, L298N motor and Bluetooth module. Sensing the temperature, with an DHT11, Arduino and Bluetooth module. Upload the code to the Arduino using the knowledge of programming. The Arduino code simulated on software and be interface with the hardware. The device can be controlled by any smart device with android. AirDroid is an app exclusive to Android which enables you to connect your device to PC through a Wi-Fi controller of wireless network. It is used to connect the mobile camera to view in our pc to fixing in the car. It also used to view the location of the car. The Robotic car sense the temperature to view by the mobile app. All the controls of the vehicle on the app on that device. It is used to sense the environment of the military force before doing some of the process. It is used for the sensing the environment of the system.","downloadable_attachments":[{"id":58607857,"asset_id":38537495,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":104799352,"first_name":"Vijayalakshmi","last_name":"Selvaraj","domain_name":"independent","page_name":"SushiSushi1","display_name":"Vijayalakshmi Selvaraj","profile_url":"https://independent.academia.edu/SushiSushi1?f_ri=34232","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":36424,"name":"Mobile Technology Applications","url":"https://www.academia.edu/Documents/in/Mobile_Technology_Applications?f_ri=34232","nofollow":true},{"id":304729,"name":"Store Location","url":"https://www.academia.edu/Documents/in/Store_Location?f_ri=34232","nofollow":true},{"id":336589,"name":"Location Analysis","url":"https://www.academia.edu/Documents/in/Location_Analysis?f_ri=34232","nofollow":true},{"id":418010,"name":"Location Tracking","url":"https://www.academia.edu/Documents/in/Location_Tracking?f_ri=34232"},{"id":881788,"name":"US ARMY SPECIAL FORCES","url":"https://www.academia.edu/Documents/in/US_ARMY_SPECIAL_FORCES?f_ri=34232"},{"id":3161015,"name":"Temperature sensing","url":"https://www.academia.edu/Documents/in/Temperature_sensing?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_7423642" data-work_id="7423642" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/7423642/IJESIT_Simulation_of_Tin_Bath">IJESIT Simulation of Tin Bath</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Flat glass is produced by the "float glass process" where molten glass is poured onto a bath of molten tin. The glass floats on the tin and levels out as it spreads along the bath. Consequently, it gives a smooth face to both sides which... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_7423642" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Flat glass is produced by the "float glass process" where molten glass is poured onto a bath of molten tin. The glass floats on the tin and levels out as it spreads along the bath. Consequently, it gives a smooth face to both sides which is then cooled and solidified into flat sheet of glass. Investigators have studied different aspects of tin bath such as fluid dynamics, thermal behavior, tin depth profiles, and diffusion of tin in glass [1-5].</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/7423642" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="2b1c08ad26dfe9ab1fd57c7d5f9337d9" rel="nofollow" data-download="{"attachment_id":34009112,"asset_id":7423642,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/34009112/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="13173101" href="https://independent.academia.edu/DJMohanty">DJ Mohanty</a><script data-card-contents-for-user="13173101" type="text/json">{"id":13173101,"first_name":"DJ","last_name":"Mohanty","domain_name":"independent","page_name":"DJMohanty","display_name":"DJ Mohanty","profile_url":"https://independent.academia.edu/DJMohanty?f_ri=34232","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_7423642 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="7423642"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 7423642, container: ".js-paper-rank-work_7423642", }); 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$(".js-view-count[data-work-id=7423642]").text(description); $(".js-view-count-work_7423642").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_7423642").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="7423642"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">13</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="1457" rel="nofollow" href="https://www.academia.edu/Documents/in/Photovoltaics">Photovoltaics</a>, <script data-card-contents-for-ri="1457" type="text/json">{"id":1457,"name":"Photovoltaics","url":"https://www.academia.edu/Documents/in/Photovoltaics?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="7742" rel="nofollow" href="https://www.academia.edu/Documents/in/Glass">Glass</a>, <script data-card-contents-for-ri="7742" type="text/json">{"id":7742,"name":"Glass","url":"https://www.academia.edu/Documents/in/Glass?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="9901" rel="nofollow" href="https://www.academia.edu/Documents/in/High_Temperature_Ceramics">High Temperature Ceramics</a>, <script data-card-contents-for-ri="9901" type="text/json">{"id":9901,"name":"High Temperature Ceramics","url":"https://www.academia.edu/Documents/in/High_Temperature_Ceramics?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="12502" rel="nofollow" href="https://www.academia.edu/Documents/in/Composite_Materials">Composite Materials</a><script data-card-contents-for-ri="12502" type="text/json">{"id":12502,"name":"Composite Materials","url":"https://www.academia.edu/Documents/in/Composite_Materials?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=7423642]'), work: {"id":7423642,"title":"IJESIT Simulation of Tin Bath","created_at":"2014-06-22T03:13:41.637-07:00","url":"https://www.academia.edu/7423642/IJESIT_Simulation_of_Tin_Bath?f_ri=34232","dom_id":"work_7423642","summary":"Flat glass is produced by the \"float glass process\" where molten glass is poured onto a bath of molten tin. The glass floats on the tin and levels out as it spreads along the bath. Consequently, it gives a smooth face to both sides which is then cooled and solidified into flat sheet of glass. Investigators have studied different aspects of tin bath such as fluid dynamics, thermal behavior, tin depth profiles, and diffusion of tin in glass [1-5].","downloadable_attachments":[{"id":34009112,"asset_id":7423642,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":13173101,"first_name":"DJ","last_name":"Mohanty","domain_name":"independent","page_name":"DJMohanty","display_name":"DJ Mohanty","profile_url":"https://independent.academia.edu/DJMohanty?f_ri=34232","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":1457,"name":"Photovoltaics","url":"https://www.academia.edu/Documents/in/Photovoltaics?f_ri=34232","nofollow":true},{"id":7742,"name":"Glass","url":"https://www.academia.edu/Documents/in/Glass?f_ri=34232","nofollow":true},{"id":9901,"name":"High Temperature Ceramics","url":"https://www.academia.edu/Documents/in/High_Temperature_Ceramics?f_ri=34232","nofollow":true},{"id":12502,"name":"Composite Materials","url":"https://www.academia.edu/Documents/in/Composite_Materials?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232"},{"id":36098,"name":"Glass \u0026 Glass-Ceramics","url":"https://www.academia.edu/Documents/in/Glass_and_Glass-Ceramics?f_ri=34232"},{"id":52432,"name":"Piezoelectric ceramics","url":"https://www.academia.edu/Documents/in/Piezoelectric_ceramics?f_ri=34232"},{"id":53910,"name":"Rare Earth Elements","url":"https://www.academia.edu/Documents/in/Rare_Earth_Elements?f_ri=34232"},{"id":103052,"name":"Ceramic thermal barrier coatings","url":"https://www.academia.edu/Documents/in/Ceramic_thermal_barrier_coatings?f_ri=34232"},{"id":119826,"name":"Aerospace materials","url":"https://www.academia.edu/Documents/in/Aerospace_materials?f_ri=34232"},{"id":157237,"name":"Self-healing materials","url":"https://www.academia.edu/Documents/in/Self-healing_materials?f_ri=34232"},{"id":165259,"name":"Piezoelectric Energy Harvesting","url":"https://www.academia.edu/Documents/in/Piezoelectric_Energy_Harvesting?f_ri=34232"},{"id":287978,"name":"advanced materials including CFRP composite for space/ aerospace application","url":"https://www.academia.edu/Documents/in/advanced_materials_including_CFRP_composite_for_space_aerospace_application?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_50238804" data-work_id="50238804" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/50238804/Master_Thesis">Master Thesis</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Strongly correlated matter have been studied since the first appearance of insulating behavior in believed conductors. The first model properly capturing electronic correlations, the Hubbard model, changed the ways we think about... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_50238804" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Strongly correlated matter have been studied since the first appearance of insulating behavior in<br />believed conductors. The first model properly capturing electronic correlations, the Hubbard<br />model, changed the ways we think about electrons in crystals. This become even more compelling<br />due to emergent novel phenomena cased by the competition of electronic, spin and orbital degrees<br />of freedom. Iron-based superconductors are a prominent example of such unique physics. Recent<br />inelastic neutron scattering experiments on iron-based ladders revealed the existence of the ↑↑↓↓<br />magnetic state. As magnetic correlations are believed to be of utmost importance in the study of<br />high-Tc superconductivity (SC), a considerable focus was put on the magnetic normal phase in<br />such systems. Years of both theoretical and experimental investigations probed magnetism in<br />low-dimensional high-Tc SC. However, the finite temperature dynamics were put aside as the<br />numerical complexity is tremendous. This study focuses on exact numerical techniques to capture<br />the whole Hilbert space, thus the calculation of thermodynamic quantities is straightforward,<br />unlike in approximate techniques. Although only small clusters can be studied, I present novel<br />results for multiorbital systems, modeled by the generalized Kondo-Heisenberg model. We show<br />evidence of the Coulomb assisted quantum phase transition from a singlet to triplet ground state.<br />Additionally we hint the possibility of fractional excitations and a spin-liquid phase at elevated<br />interaction strength.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/50238804" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="f402dc3c52c02a339a2ef698ab6b62df" rel="nofollow" data-download="{"attachment_id":68299313,"asset_id":50238804,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/68299313/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="60525351" href="https://independent.academia.edu/Rafa%C5%82%C5%9Awi%C4%99tek">Rafał Świętek</a><script data-card-contents-for-user="60525351" type="text/json">{"id":60525351,"first_name":"Rafał","last_name":"Świętek","domain_name":"independent","page_name":"RafałŚwiętek","display_name":"Rafał Świętek","profile_url":"https://independent.academia.edu/Rafa%C5%82%C5%9Awi%C4%99tek?f_ri=34232","photo":"https://0.academia-photos.com/60525351/61077272/49348700/s65_rafa_._wi_tek.png"}</script></span></span></li><li class="js-paper-rank-work_50238804 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="50238804"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 50238804, container: ".js-paper-rank-work_50238804", }); 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$(".js-view-count[data-work-id=50238804]").text(description); $(".js-view-count-work_50238804").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_50238804").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="50238804"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">3</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a>, <script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="54038" rel="nofollow" href="https://www.academia.edu/Documents/in/Low_Dimensional_Systems">Low Dimensional Systems</a>, <script data-card-contents-for-ri="54038" type="text/json">{"id":54038,"name":"Low Dimensional Systems","url":"https://www.academia.edu/Documents/in/Low_Dimensional_Systems?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="800943" rel="nofollow" href="https://www.academia.edu/Documents/in/Strongly_correlated_materials">Strongly correlated materials</a><script data-card-contents-for-ri="800943" type="text/json">{"id":800943,"name":"Strongly correlated materials","url":"https://www.academia.edu/Documents/in/Strongly_correlated_materials?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=50238804]'), work: {"id":50238804,"title":"Master Thesis","created_at":"2021-07-25T04:46:50.210-07:00","url":"https://www.academia.edu/50238804/Master_Thesis?f_ri=34232","dom_id":"work_50238804","summary":"Strongly correlated matter have been studied since the first appearance of insulating behavior in\nbelieved conductors. The first model properly capturing electronic correlations, the Hubbard\nmodel, changed the ways we think about electrons in crystals. This become even more compelling\ndue to emergent novel phenomena cased by the competition of electronic, spin and orbital degrees\nof freedom. Iron-based superconductors are a prominent example of such unique physics. Recent\ninelastic neutron scattering experiments on iron-based ladders revealed the existence of the ↑↑↓↓\nmagnetic state. As magnetic correlations are believed to be of utmost importance in the study of\nhigh-Tc superconductivity (SC), a considerable focus was put on the magnetic normal phase in\nsuch systems. Years of both theoretical and experimental investigations probed magnetism in\nlow-dimensional high-Tc SC. However, the finite temperature dynamics were put aside as the\nnumerical complexity is tremendous. This study focuses on exact numerical techniques to capture\nthe whole Hilbert space, thus the calculation of thermodynamic quantities is straightforward,\nunlike in approximate techniques. Although only small clusters can be studied, I present novel\nresults for multiorbital systems, modeled by the generalized Kondo-Heisenberg model. We show\nevidence of the Coulomb assisted quantum phase transition from a singlet to triplet ground state.\nAdditionally we hint the possibility of fractional excitations and a spin-liquid phase at elevated\ninteraction strength.","downloadable_attachments":[{"id":68299313,"asset_id":50238804,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":60525351,"first_name":"Rafał","last_name":"Świętek","domain_name":"independent","page_name":"RafałŚwiętek","display_name":"Rafał Świętek","profile_url":"https://independent.academia.edu/Rafa%C5%82%C5%9Awi%C4%99tek?f_ri=34232","photo":"https://0.academia-photos.com/60525351/61077272/49348700/s65_rafa_._wi_tek.png"}],"research_interests":[{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":54038,"name":"Low Dimensional Systems","url":"https://www.academia.edu/Documents/in/Low_Dimensional_Systems?f_ri=34232","nofollow":true},{"id":800943,"name":"Strongly correlated materials","url":"https://www.academia.edu/Documents/in/Strongly_correlated_materials?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_15169670" data-work_id="15169670" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/15169670/Book_Superconductors_New_Developments">Book: Superconductors --New Developments</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Preface Superconductivity is developing steadily and new perspective materials appear each year. Electrodynamics of superconductors is also a vigorously evolving field of science. A lot of books on superconductivity can be found in... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_15169670" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Preface <br />Superconductivity is developing steadily and new perspective materials appear each year. <br />Electrodynamics of superconductors is also a vigorously evolving field of science. A lot of books on superconductivity can be found in libraries and on Internet. This book is a collection of chapters dealing with various old and new problems of the superconducting state. It includes 8 experimental and 4 theoretical chapters written by wellknown specialists and young researchers. Oxides, pnictides, chalcogenides and intermetallic compounds are described here. The superconducting order parameter symmetry is discussed and consequences of the actual non-trivial symmetry are studied. Impurity and tunneling <br />effects are among topics covered by the chapters. <br />I hope the book will be useful for undergraduates, postgraduates and professionals. <br /> <br />Dr. Alex Gabovich <br />Institute of Physics <br />Kiev, Ukraine</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/15169670" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="ca8d207d53935a87d0e3467592db48da" rel="nofollow" data-download="{"attachment_id":38565807,"asset_id":15169670,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/38565807/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="3159343" href="https://iop-kiev.academia.edu/AlexanderGabovich">Alexander M Gabovich</a><script data-card-contents-for-user="3159343" type="text/json">{"id":3159343,"first_name":"Alexander","last_name":"Gabovich","domain_name":"iop-kiev","page_name":"AlexanderGabovich","display_name":"Alexander M Gabovich","profile_url":"https://iop-kiev.academia.edu/AlexanderGabovich?f_ri=34232","photo":"https://0.academia-photos.com/3159343/1074807/1341057/s65_alexander.gabovich.jpg"}</script></span></span></li><li class="js-paper-rank-work_15169670 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="15169670"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 15169670, container: ".js-paper-rank-work_15169670", }); });</script></li><li class="js-percentile-work_15169670 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 15169670; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_15169670"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_15169670 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="15169670"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 15169670; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=15169670]").text(description); $(".js-view-count-work_15169670").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_15169670").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="15169670"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i></div><span class="InlineList-item-text u-textTruncate u-pl6x"><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (false) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=15169670]'), work: {"id":15169670,"title":"Book: Superconductors --New Developments","created_at":"2015-08-25T06:04:36.478-07:00","url":"https://www.academia.edu/15169670/Book_Superconductors_New_Developments?f_ri=34232","dom_id":"work_15169670","summary":"Preface\r\nSuperconductivity is developing steadily and new perspective materials appear each year.\r\nElectrodynamics of superconductors is also a vigorously evolving field of science. A lot of books on superconductivity can be found in libraries and on Internet. This book is a collection of chapters dealing with various old and new problems of the superconducting state. It includes 8 experimental and 4 theoretical chapters written by wellknown specialists and young researchers. Oxides, pnictides, chalcogenides and intermetallic compounds are described here. The superconducting order parameter symmetry is discussed and consequences of the actual non-trivial symmetry are studied. Impurity and tunneling\r\neffects are among topics covered by the chapters.\r\nI hope the book will be useful for undergraduates, postgraduates and professionals.\r\n\r\nDr. Alex Gabovich\r\nInstitute of Physics\r\nKiev, Ukraine","downloadable_attachments":[{"id":38565807,"asset_id":15169670,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":3159343,"first_name":"Alexander","last_name":"Gabovich","domain_name":"iop-kiev","page_name":"AlexanderGabovich","display_name":"Alexander M Gabovich","profile_url":"https://iop-kiev.academia.edu/AlexanderGabovich?f_ri=34232","photo":"https://0.academia-photos.com/3159343/1074807/1341057/s65_alexander.gabovich.jpg"}],"research_interests":[{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_36304606" data-work_id="36304606" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/36304606/Bose_Einstein_Condensation_in_Open_Systems_Pumped_Far_Off_Classical_Thermodynamic_Equilibrium_Room_Temperature_Superconductors_and_Low_Power_Warp_Drive_Wormhole_Metric_Engineering_of_Einstein_s_Gravitational_Field_V13">Bose-Einstein Condensation in Open Systems Pumped Far Off Classical Thermodynamic Equilibrium Room Temperature Superconductors & Low Power Warp Drive/Wormhole Metric Engineering of Einstein’s Gravitational Field V13</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Jack Sarfatti <a href="mailto:adastra1@icloud.com" rel="nofollow">adastra1@icloud.com</a> Under Construction April 13, 2018 This version v13 uses a more precise notation closer to experiment in which the Frohlich pump power spectrum must be integrated over a range of frequencies and... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_36304606" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Jack Sarfatti <br /><a href="mailto:adastra1@icloud.com" rel="nofollow">adastra1@icloud.com</a> <br /> <br />Under Construction <br />April 13, 2018 <br /> <br />This version v13 uses a more precise notation closer to experiment in which the Frohlich pump power spectrum must be integrated over a range of frequencies and wave vectors. The powers of frequency and wave vectors in the integrands are determined by dimensional analysis. It also corrects an error in my dimensional analysis in v3 and adds new content on statistical mechanics and thermodynamics. The many-body Green’s function formalism is introduced for Aharonov’s two-state vector locally retrocausal quantum mechanics, but still without the Sutherland post-quantum wave action <—> Bohm particle reaction Lagrangian. The linear response generalized susceptibility of the room temperature superconductor and other non-equilibrium pumped Frohlich coherent many-particle systems is introduced. The implication for Einsteins general relativity for achieving rapid interstellar travel without time dilation is also introduced. Additional comments based on email exchange with Hal Puthoff on April 6, 2018. Appendix A on wavelet time-frequency phase space detector signal analysis added on April 9, 2018. <br />Equations using Feynman's weak field approximation to Einstein's gravity field equation are introduced for practical metric engineering. <br /> <br />Abstract <br /> <br />I present the basic equation to achieve room temperature and higher electrical superconductivity and other macro-quantum coherent effects in any many-boson system if the correct resonant coupling can be found for some range of frequencies and wave vectors even when the electromagnetic Frohlich pump is in the non-radiative near field of Glauber states of virtual photons with all three polarizations transverse and longitudinal.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/36304606" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="a2f9eeef393bef25e74ce7e0922c855c" rel="nofollow" data-download="{"attachment_id":56314153,"asset_id":36304606,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/56314153/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="690537" href="https://cornell.academia.edu/JackSarfatti">Jack Sarfatti</a><script data-card-contents-for-user="690537" type="text/json">{"id":690537,"first_name":"Jack","last_name":"Sarfatti","domain_name":"cornell","page_name":"JackSarfatti","display_name":"Jack Sarfatti","profile_url":"https://cornell.academia.edu/JackSarfatti?f_ri=34232","photo":"https://0.academia-photos.com/690537/870624/163601433/s65_jack.sarfatti.jpg"}</script></span></span></li><li class="js-paper-rank-work_36304606 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="36304606"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 36304606, container: ".js-paper-rank-work_36304606", }); 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$(".js-view-count[data-work-id=36304606]").text(description); $(".js-view-count-work_36304606").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_36304606").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="36304606"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">20</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="49" rel="nofollow" href="https://www.academia.edu/Documents/in/Electrical_Engineering">Electrical Engineering</a>, <script data-card-contents-for-ri="49" type="text/json">{"id":49,"name":"Electrical Engineering","url":"https://www.academia.edu/Documents/in/Electrical_Engineering?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="88" rel="nofollow" href="https://www.academia.edu/Documents/in/Aerospace_Engineering">Aerospace Engineering</a>, <script data-card-contents-for-ri="88" type="text/json">{"id":88,"name":"Aerospace Engineering","url":"https://www.academia.edu/Documents/in/Aerospace_Engineering?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="318" rel="nofollow" href="https://www.academia.edu/Documents/in/Mathematical_Physics">Mathematical Physics</a>, <script data-card-contents-for-ri="318" type="text/json">{"id":318,"name":"Mathematical Physics","url":"https://www.academia.edu/Documents/in/Mathematical_Physics?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="444" rel="nofollow" href="https://www.academia.edu/Documents/in/Quantum_Computing">Quantum Computing</a><script data-card-contents-for-ri="444" type="text/json">{"id":444,"name":"Quantum Computing","url":"https://www.academia.edu/Documents/in/Quantum_Computing?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=36304606]'), work: {"id":36304606,"title":"Bose-Einstein Condensation in Open Systems \r\nPumped Far Off Classical Thermodynamic Equilibrium\r\nRoom Temperature Superconductors \u0026 Low Power Warp Drive/Wormhole Metric Engineering of Einstein’s Gravitational Field V13","created_at":"2018-04-01T12:49:26.814-07:00","url":"https://www.academia.edu/36304606/Bose_Einstein_Condensation_in_Open_Systems_Pumped_Far_Off_Classical_Thermodynamic_Equilibrium_Room_Temperature_Superconductors_and_Low_Power_Warp_Drive_Wormhole_Metric_Engineering_of_Einstein_s_Gravitational_Field_V13?f_ri=34232","dom_id":"work_36304606","summary":"\r\nJack Sarfatti\r\nadastra1@icloud.com\r\n\r\nUnder Construction \r\nApril 13, 2018\r\n\r\nThis version v13 uses a more precise notation closer to experiment in which the Frohlich pump power spectrum must be integrated over a range of frequencies and wave vectors. The powers of frequency and wave vectors in the integrands are determined by dimensional analysis. It also corrects an error in my dimensional analysis in v3 and adds new content on statistical mechanics and thermodynamics. The many-body Green’s function formalism is introduced for Aharonov’s two-state vector locally retrocausal quantum mechanics, but still without the Sutherland post-quantum wave action \u003c—\u003e Bohm particle reaction Lagrangian. The linear response generalized susceptibility of the room temperature superconductor and other non-equilibrium pumped Frohlich coherent many-particle systems is introduced. The implication for Einsteins general relativity for achieving rapid interstellar travel without time dilation is also introduced. Additional comments based on email exchange with Hal Puthoff on April 6, 2018. Appendix A on wavelet time-frequency phase space detector signal analysis added on April 9, 2018.\r\nEquations using Feynman's weak field approximation to Einstein's gravity field equation are introduced for practical metric engineering.\r\n\r\nAbstract\r\n\r\nI present the basic equation to achieve room temperature and higher electrical superconductivity and other macro-quantum coherent effects in any many-boson system if the correct resonant coupling can be found for some range of frequencies and wave vectors even when the electromagnetic Frohlich pump is in the non-radiative near field of Glauber states of virtual photons with all three polarizations transverse and longitudinal.\r\n","downloadable_attachments":[{"id":56314153,"asset_id":36304606,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":690537,"first_name":"Jack","last_name":"Sarfatti","domain_name":"cornell","page_name":"JackSarfatti","display_name":"Jack Sarfatti","profile_url":"https://cornell.academia.edu/JackSarfatti?f_ri=34232","photo":"https://0.academia-photos.com/690537/870624/163601433/s65_jack.sarfatti.jpg"}],"research_interests":[{"id":49,"name":"Electrical Engineering","url":"https://www.academia.edu/Documents/in/Electrical_Engineering?f_ri=34232","nofollow":true},{"id":88,"name":"Aerospace Engineering","url":"https://www.academia.edu/Documents/in/Aerospace_Engineering?f_ri=34232","nofollow":true},{"id":318,"name":"Mathematical Physics","url":"https://www.academia.edu/Documents/in/Mathematical_Physics?f_ri=34232","nofollow":true},{"id":444,"name":"Quantum Computing","url":"https://www.academia.edu/Documents/in/Quantum_Computing?f_ri=34232","nofollow":true},{"id":503,"name":"Theoretical Physics","url":"https://www.academia.edu/Documents/in/Theoretical_Physics?f_ri=34232"},{"id":518,"name":"Quantum Physics","url":"https://www.academia.edu/Documents/in/Quantum_Physics?f_ri=34232"},{"id":522,"name":"Thermodynamics","url":"https://www.academia.edu/Documents/in/Thermodynamics?f_ri=34232"},{"id":2640,"name":"Quantum Information","url":"https://www.academia.edu/Documents/in/Quantum_Information?f_ri=34232"},{"id":2696,"name":"Power Electronics","url":"https://www.academia.edu/Documents/in/Power_Electronics?f_ri=34232"},{"id":5748,"name":"Power System","url":"https://www.academia.edu/Documents/in/Power_System?f_ri=34232"},{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232"},{"id":10092,"name":"Quantum Field Theory","url":"https://www.academia.edu/Documents/in/Quantum_Field_Theory?f_ri=34232"},{"id":19204,"name":"Nonequilibrium statistical mechanics","url":"https://www.academia.edu/Documents/in/Nonequilibrium_statistical_mechanics?f_ri=34232"},{"id":22983,"name":"Electrical","url":"https://www.academia.edu/Documents/in/Electrical?f_ri=34232"},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232"},{"id":34234,"name":"Electrical and Electronics","url":"https://www.academia.edu/Documents/in/Electrical_and_Electronics?f_ri=34232"},{"id":34819,"name":"Electric Power Systems","url":"https://www.academia.edu/Documents/in/Electric_Power_Systems?f_ri=34232"},{"id":38253,"name":"Power Electrical Engineering","url":"https://www.academia.edu/Documents/in/Power_Electrical_Engineering?f_ri=34232"},{"id":125513,"name":"Superconductors","url":"https://www.academia.edu/Documents/in/Superconductors?f_ri=34232"},{"id":1224548,"name":"Electrical and Computer Engineering (ECE)","url":"https://www.academia.edu/Documents/in/Electrical_and_Computer_Engineering_ECE_?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_38455294" data-work_id="38455294" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/38455294/High_Temperature_Superconductivity_in_the_Cuprates_Materials_Phenomena_and_a_Mechanism">High Temperature Superconductivity in the Cuprates: Materials, Phenomena and a Mechanism</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Superconductivity in the cuprates, discovered in the late 1980s and occurring at unprecedentedly high temperatures (up to about 140K) in about thirty chemically distinct families, continues to be a major problem in physics. In this... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_38455294" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Superconductivity in the cuprates, discovered in the late 1980s and occurring at unprecedentedly high temperatures (up<br />to about 140K) in about thirty chemically distinct families, continues to be a major problem in physics. In this article, after a brief<br />introduction of these square planar materials with weak interlayer coupling, we mention some of the salient electronic properties<br />of hole doped cuprates such as the pseudogap phase and the Fermi arc . We then outline a phenomenological, Ginzburg Landau<br />like theory developed by some of us for the emergent d-wave symmetry superconductivity in these materials, and confronted successfully with a large amount of experimental information. A more recent application of the approach to fluctuation diamagnetism<br />and to the anomalously large Nernst effect is also discussed.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/38455294" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="41ac23080803db861e3fbc08956bf093" rel="nofollow" data-download="{"attachment_id":58518717,"asset_id":38455294,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/58518717/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="98699526" href="https://vit.academia.edu/KingshukSarkar">Kingshuk Sarkar</a><script data-card-contents-for-user="98699526" type="text/json">{"id":98699526,"first_name":"Kingshuk","last_name":"Sarkar","domain_name":"vit","page_name":"KingshukSarkar","display_name":"Kingshuk Sarkar","profile_url":"https://vit.academia.edu/KingshukSarkar?f_ri=34232","photo":"https://0.academia-photos.com/98699526/22996997/22126497/s65_kingshuk.sarkar.jpg"}</script></span></span></li><li class="js-paper-rank-work_38455294 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="38455294"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 38455294, container: ".js-paper-rank-work_38455294", }); });</script></li><li class="js-percentile-work_38455294 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 38455294; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_38455294"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_38455294 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="38455294"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 38455294; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=38455294]").text(description); $(".js-view-count-work_38455294").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_38455294").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="38455294"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i></div><span class="InlineList-item-text u-textTruncate u-pl6x"><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (false) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=38455294]'), work: {"id":38455294,"title":"High Temperature Superconductivity in the Cuprates: Materials, Phenomena and a Mechanism","created_at":"2019-02-28T04:55:42.907-08:00","url":"https://www.academia.edu/38455294/High_Temperature_Superconductivity_in_the_Cuprates_Materials_Phenomena_and_a_Mechanism?f_ri=34232","dom_id":"work_38455294","summary":"Superconductivity in the cuprates, discovered in the late 1980s and occurring at unprecedentedly high temperatures (up\nto about 140K) in about thirty chemically distinct families, continues to be a major problem in physics. In this article, after a brief\nintroduction of these square planar materials with weak interlayer coupling, we mention some of the salient electronic properties\nof hole doped cuprates such as the pseudogap phase and the Fermi arc . We then outline a phenomenological, Ginzburg Landau\nlike theory developed by some of us for the emergent d-wave symmetry superconductivity in these materials, and confronted successfully with a large amount of experimental information. A more recent application of the approach to fluctuation diamagnetism\nand to the anomalously large Nernst effect is also discussed.","downloadable_attachments":[{"id":58518717,"asset_id":38455294,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":98699526,"first_name":"Kingshuk","last_name":"Sarkar","domain_name":"vit","page_name":"KingshukSarkar","display_name":"Kingshuk Sarkar","profile_url":"https://vit.academia.edu/KingshukSarkar?f_ri=34232","photo":"https://0.academia-photos.com/98699526/22996997/22126497/s65_kingshuk.sarkar.jpg"}],"research_interests":[{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_1129176" data-work_id="1129176" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/1129176/The_comaptibility_of_Zhang_Rice_singlets_and_Spin_Glasses">The comaptibility of Zhang-Rice singlets and Spin Glasses</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">To address the incompatibility of Zhang-Rice singlet formation and the observed spin glass behavior, an effective model is proposed for the electronic behavior of cuprate materials. The model includes an antiferromagnetic interaction... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_1129176" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">To address the incompatibility of Zhang-Rice singlet formation and the observed spin glass behavior, an effective model is proposed for the electronic behavior of cuprate materials. The model includes an antiferromagnetic interaction between the spin of the hole in a Zhang-Rice orbital and the spin of the hole on the corresponding copper site. While in the large interaction limit this recovers the t-J model, in the low energy limit the Zhang-Rice singlets are deformed. It is also shown that such deformation can induce random defect ferromagnetic (FM) bonds between adjacent local spins, an effect herein referred to as unusual double exchange, and then spin glass behavior shall result in the case of localized holes. A derivation of the model is also presented.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/1129176" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="2271255751fe964275355943bd1cea27" rel="nofollow" data-download="{"attachment_id":6976193,"asset_id":1129176,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/6976193/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="100272" href="https://manchester.academia.edu/HaiYaoDENG">Hai-Yao DENG</a><script data-card-contents-for-user="100272" type="text/json">{"id":100272,"first_name":"Hai-Yao","last_name":"DENG","domain_name":"manchester","page_name":"HaiYaoDENG","display_name":"Hai-Yao DENG","profile_url":"https://manchester.academia.edu/HaiYaoDENG?f_ri=34232","photo":"https://0.academia-photos.com/100272/27632/25446/s65_hai-yao.deng.jpg"}</script></span></span></li><li class="js-paper-rank-work_1129176 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="1129176"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 1129176, container: ".js-paper-rank-work_1129176", }); });</script></li><li class="js-percentile-work_1129176 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1129176; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_1129176"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_1129176 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="1129176"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1129176; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1129176]").text(description); $(".js-view-count-work_1129176").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_1129176").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="1129176"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">5</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="16400" rel="nofollow" href="https://www.academia.edu/Documents/in/Disordered_Systems">Disordered Systems</a>, <script data-card-contents-for-ri="16400" type="text/json">{"id":16400,"name":"Disordered Systems","url":"https://www.academia.edu/Documents/in/Disordered_Systems?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a>, <script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="99109" rel="nofollow" href="https://www.academia.edu/Documents/in/Cuprate_Superconductors">Cuprate Superconductors</a>, <script data-card-contents-for-ri="99109" type="text/json">{"id":99109,"name":"Cuprate Superconductors","url":"https://www.academia.edu/Documents/in/Cuprate_Superconductors?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="339316" rel="nofollow" href="https://www.academia.edu/Documents/in/Spin_Glass">Spin Glass</a><script data-card-contents-for-ri="339316" type="text/json">{"id":339316,"name":"Spin Glass","url":"https://www.academia.edu/Documents/in/Spin_Glass?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=1129176]'), work: {"id":1129176,"title":"The comaptibility of Zhang-Rice singlets and Spin Glasses","created_at":"2011-12-01T11:46:46.481-08:00","url":"https://www.academia.edu/1129176/The_comaptibility_of_Zhang_Rice_singlets_and_Spin_Glasses?f_ri=34232","dom_id":"work_1129176","summary":"To address the incompatibility of Zhang-Rice singlet formation and the observed spin glass behavior, an effective model is proposed for the electronic behavior of cuprate materials. The model includes an antiferromagnetic interaction between the spin of the hole in a Zhang-Rice orbital and the spin of the hole on the corresponding copper site. While in the large interaction limit this recovers the t-J model, in the low energy limit the Zhang-Rice singlets are deformed. It is also shown that such deformation can induce random defect ferromagnetic (FM) bonds between adjacent local spins, an effect herein referred to as unusual double exchange, and then spin glass behavior shall result in the case of localized holes. A derivation of the model is also presented.","downloadable_attachments":[{"id":6976193,"asset_id":1129176,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":100272,"first_name":"Hai-Yao","last_name":"DENG","domain_name":"manchester","page_name":"HaiYaoDENG","display_name":"Hai-Yao DENG","profile_url":"https://manchester.academia.edu/HaiYaoDENG?f_ri=34232","photo":"https://0.academia-photos.com/100272/27632/25446/s65_hai-yao.deng.jpg"}],"research_interests":[{"id":16400,"name":"Disordered Systems","url":"https://www.academia.edu/Documents/in/Disordered_Systems?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":99109,"name":"Cuprate Superconductors","url":"https://www.academia.edu/Documents/in/Cuprate_Superconductors?f_ri=34232","nofollow":true},{"id":339316,"name":"Spin Glass","url":"https://www.academia.edu/Documents/in/Spin_Glass?f_ri=34232","nofollow":true},{"id":339318,"name":"Carrier Localization","url":"https://www.academia.edu/Documents/in/Carrier_Localization?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_10399835" data-work_id="10399835" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/10399835/Pseudogap_from_ARPES_experiment_three_gaps_in_cuprates_and_topological_superconductivity">Pseudogap from ARPES experiment: three gaps in cuprates and topological superconductivity</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">A term first coined by Mott back in 1968 a `pseudogap' is the depletion of the electronic density of states at the Fermi level, and pseudogaps have been observed in many systems. However, since the discovery of the high temperature... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_10399835" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">A term first coined by Mott back in 1968 a `pseudogap' is the depletion of the electronic density of states at the Fermi level, and pseudogaps have been observed in many systems. However, since the discovery of the high temperature superconductors (HTSC) in 1986, the central role attributed to the pseudogap in these systems has meant that by many researchers now associate the term pseudogap exclusively with the HTSC phenomenon. Recently, the problem has got a lot of new attention with the rediscovery of two distinct energy scales (`two-gap scenario') and charge density waves patterns in the cuprates. Despite many excellent reviews on the pseudogap phenomenon in HTSC, published from its very discovery up to now, the mechanism of the pseudogap and its relation to superconductivity are still open questions. The present review represents a contribution dealing with the pseudogap, focusing on results from angle resolved photoemission spectroscopy (ARPES) and ends up with the conclusion that the pseudogap in cuprates is a complex phenomenon which includes at least three different `intertwined' orders: spin and charge density waves and preformed pairs, which appears in different parts of the phase diagram. The density waves in cuprates are competing to superconductivity for the electronic states but, on the other hand, should drive the electronic structure to vicinity of Lifshitz transition, that could be a key similarity between the superconducting cuprates and iron based superconductors. One may also note that since the pseudogap in cuprates has multiple origins there is no need to recoin the term suggested by Mott.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/10399835" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="7d48e1c45f4e9590ccd1fd6acf569147" rel="nofollow" data-download="{"attachment_id":36454447,"asset_id":10399835,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/36454447/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="22769033" href="https://independent.academia.edu/AlexanderKordyuk">Alexander Kordyuk</a><script data-card-contents-for-user="22769033" type="text/json">{"id":22769033,"first_name":"Alexander","last_name":"Kordyuk","domain_name":"independent","page_name":"AlexanderKordyuk","display_name":"Alexander Kordyuk","profile_url":"https://independent.academia.edu/AlexanderKordyuk?f_ri=34232","photo":"https://gravatar.com/avatar/3f87bce5d32ba67d364010ee6c6fc712?s=65"}</script></span></span></li><li class="js-paper-rank-work_10399835 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="10399835"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 10399835, container: ".js-paper-rank-work_10399835", }); 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$(".js-view-count[data-work-id=10399835]").text(description); $(".js-view-count-work_10399835").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_10399835").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="10399835"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">8</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="6469" rel="nofollow" href="https://www.academia.edu/Documents/in/Superconductivity">Superconductivity</a>, <script data-card-contents-for-ri="6469" type="text/json">{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="32736" rel="nofollow" href="https://www.academia.edu/Documents/in/ARPES">ARPES</a>, <script data-card-contents-for-ri="32736" type="text/json">{"id":32736,"name":"ARPES","url":"https://www.academia.edu/Documents/in/ARPES?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a>, <script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="99109" rel="nofollow" href="https://www.academia.edu/Documents/in/Cuprate_Superconductors">Cuprate Superconductors</a><script data-card-contents-for-ri="99109" type="text/json">{"id":99109,"name":"Cuprate Superconductors","url":"https://www.academia.edu/Documents/in/Cuprate_Superconductors?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=10399835]'), work: {"id":10399835,"title":"Pseudogap from ARPES experiment: three gaps in cuprates and topological superconductivity","created_at":"2015-01-30T15:57:08.408-08:00","url":"https://www.academia.edu/10399835/Pseudogap_from_ARPES_experiment_three_gaps_in_cuprates_and_topological_superconductivity?f_ri=34232","dom_id":"work_10399835","summary":"A term first coined by Mott back in 1968 a `pseudogap' is the depletion of the electronic density of states at the Fermi level, and pseudogaps have been observed in many systems. However, since the discovery of the high temperature superconductors (HTSC) in 1986, the central role attributed to the pseudogap in these systems has meant that by many researchers now associate the term pseudogap exclusively with the HTSC phenomenon. Recently, the problem has got a lot of new attention with the rediscovery of two distinct energy scales (`two-gap scenario') and charge density waves patterns in the cuprates. Despite many excellent reviews on the pseudogap phenomenon in HTSC, published from its very discovery up to now, the mechanism of the pseudogap and its relation to superconductivity are still open questions. The present review represents a contribution dealing with the pseudogap, focusing on results from angle resolved photoemission spectroscopy (ARPES) and ends up with the conclusion that the pseudogap in cuprates is a complex phenomenon which includes at least three different `intertwined' orders: spin and charge density waves and preformed pairs, which appears in different parts of the phase diagram. The density waves in cuprates are competing to superconductivity for the electronic states but, on the other hand, should drive the electronic structure to vicinity of Lifshitz transition, that could be a key similarity between the superconducting cuprates and iron based superconductors. One may also note that since the pseudogap in cuprates has multiple origins there is no need to recoin the term suggested by Mott.","downloadable_attachments":[{"id":36454447,"asset_id":10399835,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":22769033,"first_name":"Alexander","last_name":"Kordyuk","domain_name":"independent","page_name":"AlexanderKordyuk","display_name":"Alexander Kordyuk","profile_url":"https://independent.academia.edu/AlexanderKordyuk?f_ri=34232","photo":"https://gravatar.com/avatar/3f87bce5d32ba67d364010ee6c6fc712?s=65"}],"research_interests":[{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true},{"id":32736,"name":"ARPES","url":"https://www.academia.edu/Documents/in/ARPES?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":99109,"name":"Cuprate Superconductors","url":"https://www.academia.edu/Documents/in/Cuprate_Superconductors?f_ri=34232","nofollow":true},{"id":179371,"name":"Pseudogap","url":"https://www.academia.edu/Documents/in/Pseudogap?f_ri=34232"},{"id":210333,"name":"Photoemission Spectroscopy","url":"https://www.academia.edu/Documents/in/Photoemission_Spectroscopy?f_ri=34232"},{"id":491112,"name":"Intermetallics, Charge-Density Waves, Structural Transition","url":"https://www.academia.edu/Documents/in/Intermetallics_Charge-Density_Waves_Structural_Transition?f_ri=34232"},{"id":577264,"name":"Electronic band structure","url":"https://www.academia.edu/Documents/in/Electronic_band_structure?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_40307326" data-work_id="40307326" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/40307326/Superconductivity_in_Organic_Materials">Superconductivity in Organic Materials</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">In this paper, the development and present status of organic superconductors of charge-transfer salt based on electron donor molecules, electron acceptor molecules as well as polycyclic aromatic hydrocarbons (Tc=33K at ambient pressure),... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_40307326" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">In this paper, the development and present status of organic superconductors of charge-transfer salt based on electron donor molecules, electron acceptor molecules as well as polycyclic aromatic hydrocarbons (Tc=33K at ambient pressure), graphite (Tc=15.1K at 7.5GPa), carbon nanotube (Tc=15K in zeolite), fullerene (Tc=38K at 0.7GPa), Single component organic compound ((Tc≤2.3K at 58GPa), B doped diamond (Tc=10K) etc are discussed. The highest critical temperature obtained for an organic superconductor is 117 K which was found for hole doped C60 intercalated with CHBr3. The search for higher critical temperatures in organic superconductors appears promising.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/40307326" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="287ddca318a0932bb5b80d6cc6615f10" rel="nofollow" data-download="{"attachment_id":60548316,"asset_id":40307326,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/60548316/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="39660973" href="https://dbbtcoc.academia.edu/ShailajKumarShrivastava">Shailaj Kumar Shrivastava</a><script data-card-contents-for-user="39660973" type="text/json">{"id":39660973,"first_name":"Shailaj Kumar","last_name":"Shrivastava","domain_name":"dbbtcoc","page_name":"ShailajKumarShrivastava","display_name":"Shailaj Kumar Shrivastava","profile_url":"https://dbbtcoc.academia.edu/ShailajKumarShrivastava?f_ri=34232","photo":"https://0.academia-photos.com/39660973/14421391/158749700/s65_shailaj_kumar.shrivastava.jpg"}</script></span></span></li><li class="js-paper-rank-work_40307326 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="40307326"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 40307326, container: ".js-paper-rank-work_40307326", }); 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$(".js-view-count[data-work-id=40307326]").text(description); $(".js-view-count-work_40307326").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_40307326").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="40307326"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i></div><span class="InlineList-item-text u-textTruncate u-pl6x"><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (false) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=40307326]'), work: {"id":40307326,"title":"Superconductivity in Organic Materials","created_at":"2019-09-10T07:11:01.933-07:00","url":"https://www.academia.edu/40307326/Superconductivity_in_Organic_Materials?f_ri=34232","dom_id":"work_40307326","summary":"In this paper, the development and present status of organic superconductors of charge-transfer salt based on electron donor molecules, electron acceptor molecules as well as polycyclic aromatic hydrocarbons (Tc=33K at ambient pressure), graphite (Tc=15.1K at 7.5GPa), carbon nanotube (Tc=15K in zeolite), fullerene (Tc=38K at 0.7GPa), Single component organic compound ((Tc≤2.3K at 58GPa), B doped diamond (Tc=10K) etc are discussed. The highest critical temperature obtained for an organic superconductor is 117 K which was found for hole doped C60 intercalated with CHBr3. The search for higher critical temperatures in organic superconductors appears promising.","downloadable_attachments":[{"id":60548316,"asset_id":40307326,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":39660973,"first_name":"Shailaj Kumar","last_name":"Shrivastava","domain_name":"dbbtcoc","page_name":"ShailajKumarShrivastava","display_name":"Shailaj Kumar Shrivastava","profile_url":"https://dbbtcoc.academia.edu/ShailajKumarShrivastava?f_ri=34232","photo":"https://0.academia-photos.com/39660973/14421391/158749700/s65_shailaj_kumar.shrivastava.jpg"}],"research_interests":[{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_36636336" data-work_id="36636336" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/36636336/CRYSTAL_STRUCTURES_OF_CUPRATE_BASED_SUPERCONDUCTING_MATERIALS">CRYSTAL STRUCTURES OF CUPRATE BASED SUPERCONDUCTING MATERIALS</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">The high-T c cuprate superconductors have their structure derived from ideal perovskite structure, either through an intergrowth phenomenon or by an ordered removal of oxygen atoms. The common features of the cuprate superconductors are... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_36636336" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">The high-T c cuprate superconductors have their structure derived from ideal perovskite structure, either through an intergrowth phenomenon or by an ordered removal of oxygen atoms. The common features of the cuprate superconductors are their layered crystal structure consisting of one or more CuO 2 layers. The tetragonal cuprate superconductors shows small difference in lattice parameters a and b close to 0.38nm because of common structural features of the CuO 2 planes. In this paper, the crystal structures of cuprate based superconductors are discussed</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/36636336" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="ca2d3fe6f7958a80ea70c7e44108a6f3" rel="nofollow" data-download="{"attachment_id":56568245,"asset_id":36636336,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/56568245/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="39660973" href="https://dbbtcoc.academia.edu/ShailajKumarShrivastava">Shailaj Kumar Shrivastava</a><script data-card-contents-for-user="39660973" type="text/json">{"id":39660973,"first_name":"Shailaj Kumar","last_name":"Shrivastava","domain_name":"dbbtcoc","page_name":"ShailajKumarShrivastava","display_name":"Shailaj Kumar Shrivastava","profile_url":"https://dbbtcoc.academia.edu/ShailajKumarShrivastava?f_ri=34232","photo":"https://0.academia-photos.com/39660973/14421391/158749700/s65_shailaj_kumar.shrivastava.jpg"}</script></span></span></li><li class="js-paper-rank-work_36636336 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="36636336"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 36636336, container: ".js-paper-rank-work_36636336", }); });</script></li><li class="js-percentile-work_36636336 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 36636336; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_36636336"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_36636336 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="36636336"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 36636336; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=36636336]").text(description); $(".js-view-count-work_36636336").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_36636336").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="36636336"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i></div><span class="InlineList-item-text u-textTruncate u-pl6x"><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (false) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=36636336]'), work: {"id":36636336,"title":"CRYSTAL STRUCTURES OF CUPRATE BASED SUPERCONDUCTING MATERIALS","created_at":"2018-05-14T21:04:56.416-07:00","url":"https://www.academia.edu/36636336/CRYSTAL_STRUCTURES_OF_CUPRATE_BASED_SUPERCONDUCTING_MATERIALS?f_ri=34232","dom_id":"work_36636336","summary":"The high-T c cuprate superconductors have their structure derived from ideal perovskite structure, either through an intergrowth phenomenon or by an ordered removal of oxygen atoms. The common features of the cuprate superconductors are their layered crystal structure consisting of one or more CuO 2 layers. The tetragonal cuprate superconductors shows small difference in lattice parameters a and b close to 0.38nm because of common structural features of the CuO 2 planes. In this paper, the crystal structures of cuprate based superconductors are discussed","downloadable_attachments":[{"id":56568245,"asset_id":36636336,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":39660973,"first_name":"Shailaj Kumar","last_name":"Shrivastava","domain_name":"dbbtcoc","page_name":"ShailajKumarShrivastava","display_name":"Shailaj Kumar Shrivastava","profile_url":"https://dbbtcoc.academia.edu/ShailajKumarShrivastava?f_ri=34232","photo":"https://0.academia-photos.com/39660973/14421391/158749700/s65_shailaj_kumar.shrivastava.jpg"}],"research_interests":[{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_12878285" data-work_id="12878285" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/12878285/Pseudogap_from_ARPES_experiment_Three_gaps_in_cuprates_and_topological_superconductivity_Review_Article_">Pseudogap from ARPES experiment: Three gaps in cuprates and topological superconductivity (Review Article)</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">A term first coined by Mott back in 1968 a “pseudogap” is the depletion of the electronic density of states at the Fermi level, and pseudogaps have been observed in many systems. However, since the discovery of the high-temperature... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_12878285" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">A term first coined by Mott back in 1968 a “pseudogap” is the depletion of the electronic density of states at the Fermi level, and pseudogaps have been observed in many systems. However, since the discovery of the high-temperature superconductors (HTSC) in 1986, the central role attributed to the pseudogap in these systems has meant that by many researchers now associate the term pseudogap exclusively with the HTSC phenomenon. Recently, the problem has got a lot of new attention with the rediscovery of two distinct energy scales (“two-gap scenario”) and charge density waves patterns in the cuprates. Despite many excellent reviews on the pseudogap phenomenon in HTSC, published from its very discovery up to now, the mechanism of the pseudogap and its relation to superconductivity are still open questions. The present review represents a contribution dealing with the pseudogap, focusing on results from angle resolved photoemission spectroscopy (ARPES) and ends up with the conclusion that the pseudogap in cuprates is a complex phenomenon which includes at least three different “intertwined” orders: spin and charge density waves and preformed pairs, which appears in different parts of the phase diagram. The density waves in cuprates are competing to superconductivity for the electronic states but, on the other hand, should drive the electronic structure to vicinity of Lifshitz transition, that could be a key similarity between the superconducting cuprates and iron-based superconductors. One may also note that since the pseudogap in cuprates has multiple origins there is no need to recoin the term suggested by Mott.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/12878285" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="197da235247deffa00073a5496883c34" rel="nofollow" data-download="{"attachment_id":37861809,"asset_id":12878285,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/37861809/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="22769033" href="https://independent.academia.edu/AlexanderKordyuk">Alexander Kordyuk</a><script data-card-contents-for-user="22769033" type="text/json">{"id":22769033,"first_name":"Alexander","last_name":"Kordyuk","domain_name":"independent","page_name":"AlexanderKordyuk","display_name":"Alexander Kordyuk","profile_url":"https://independent.academia.edu/AlexanderKordyuk?f_ri=34232","photo":"https://gravatar.com/avatar/3f87bce5d32ba67d364010ee6c6fc712?s=65"}</script></span></span></li><li class="js-paper-rank-work_12878285 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="12878285"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 12878285, container: ".js-paper-rank-work_12878285", }); 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$(".js-view-count[data-work-id=12878285]").text(description); $(".js-view-count-work_12878285").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_12878285").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="12878285"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">23</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="6469" rel="nofollow" href="https://www.academia.edu/Documents/in/Superconductivity">Superconductivity</a>, <script data-card-contents-for-ri="6469" type="text/json">{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="9339" rel="nofollow" href="https://www.academia.edu/Documents/in/Raman_Spectroscopy">Raman Spectroscopy</a>, <script data-card-contents-for-ri="9339" type="text/json">{"id":9339,"name":"Raman Spectroscopy","url":"https://www.academia.edu/Documents/in/Raman_Spectroscopy?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="32736" rel="nofollow" href="https://www.academia.edu/Documents/in/ARPES">ARPES</a>, <script data-card-contents-for-ri="32736" type="text/json">{"id":32736,"name":"ARPES","url":"https://www.academia.edu/Documents/in/ARPES?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=12878285]'), work: {"id":12878285,"title":"Pseudogap from ARPES experiment: Three gaps in cuprates and topological superconductivity (Review Article)","created_at":"2015-06-08T23:41:14.450-07:00","url":"https://www.academia.edu/12878285/Pseudogap_from_ARPES_experiment_Three_gaps_in_cuprates_and_topological_superconductivity_Review_Article_?f_ri=34232","dom_id":"work_12878285","summary":"A term first coined by Mott back in 1968 a “pseudogap” is the depletion of the electronic density of states at the Fermi level, and pseudogaps have been observed in many systems. However, since the discovery of the high-temperature superconductors (HTSC) in 1986, the central role attributed to the pseudogap in these systems has meant that by many researchers now associate the term pseudogap exclusively with the HTSC phenomenon. Recently, the problem has got a lot of new attention with the rediscovery of two distinct energy scales (“two-gap scenario”) and charge density waves patterns in the cuprates. Despite many excellent reviews on the pseudogap phenomenon in HTSC, published from its very discovery up to now, the mechanism of the pseudogap and its relation to superconductivity are still open questions. The present review represents a contribution dealing with the pseudogap, focusing on results from angle resolved photoemission spectroscopy (ARPES) and ends up with the conclusion that the pseudogap in cuprates is a complex phenomenon which includes at least three different “intertwined” orders: spin and charge density waves and preformed pairs, which appears in different parts of the phase diagram. The density waves in cuprates are competing to superconductivity for the electronic states but, on the other hand, should drive the electronic structure to vicinity of Lifshitz transition, that could be a key similarity between the superconducting cuprates and iron-based superconductors. One may also note that since the pseudogap in cuprates has multiple origins there is no need to recoin the term suggested by Mott.","downloadable_attachments":[{"id":37861809,"asset_id":12878285,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":22769033,"first_name":"Alexander","last_name":"Kordyuk","domain_name":"independent","page_name":"AlexanderKordyuk","display_name":"Alexander Kordyuk","profile_url":"https://independent.academia.edu/AlexanderKordyuk?f_ri=34232","photo":"https://gravatar.com/avatar/3f87bce5d32ba67d364010ee6c6fc712?s=65"}],"research_interests":[{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true},{"id":9339,"name":"Raman Spectroscopy","url":"https://www.academia.edu/Documents/in/Raman_Spectroscopy?f_ri=34232","nofollow":true},{"id":32736,"name":"ARPES","url":"https://www.academia.edu/Documents/in/ARPES?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":50105,"name":"Scanning tunneling microscopy","url":"https://www.academia.edu/Documents/in/Scanning_tunneling_microscopy?f_ri=34232"},{"id":59221,"name":"Phase Diagrams","url":"https://www.academia.edu/Documents/in/Phase_Diagrams?f_ri=34232"},{"id":82231,"name":"Inelastic Neutron Scattering","url":"https://www.academia.edu/Documents/in/Inelastic_Neutron_Scattering?f_ri=34232"},{"id":88255,"name":"Mott metal-insulator transition","url":"https://www.academia.edu/Documents/in/Mott_metal-insulator_transition?f_ri=34232"},{"id":99109,"name":"Cuprate Superconductors","url":"https://www.academia.edu/Documents/in/Cuprate_Superconductors?f_ri=34232"},{"id":125513,"name":"Superconductors","url":"https://www.academia.edu/Documents/in/Superconductors?f_ri=34232"},{"id":179371,"name":"Pseudogap","url":"https://www.academia.edu/Documents/in/Pseudogap?f_ri=34232"},{"id":191577,"name":"Resistivity","url":"https://www.academia.edu/Documents/in/Resistivity?f_ri=34232"},{"id":219635,"name":"Electronic Structure","url":"https://www.academia.edu/Documents/in/Electronic_Structure?f_ri=34232"},{"id":332962,"name":"Angle-resolved photoemission spectroscopy","url":"https://www.academia.edu/Documents/in/Angle-resolved_photoemission_spectroscopy?f_ri=34232"},{"id":566287,"name":"Infrared absorption spectroscopy","url":"https://www.academia.edu/Documents/in/Infrared_absorption_spectroscopy?f_ri=34232"},{"id":656953,"name":"Transition Metal Dichalcogenides","url":"https://www.academia.edu/Documents/in/Transition_Metal_Dichalcogenides?f_ri=34232"},{"id":800909,"name":"RIXS","url":"https://www.academia.edu/Documents/in/RIXS?f_ri=34232"},{"id":832541,"name":"Quantum Critical Point","url":"https://www.academia.edu/Documents/in/Quantum_Critical_Point?f_ri=34232"},{"id":1927319,"name":"CDW","url":"https://www.academia.edu/Documents/in/CDW?f_ri=34232"},{"id":1938233,"name":"Charge Density Waves","url":"https://www.academia.edu/Documents/in/Charge_Density_Waves?f_ri=34232"},{"id":1958063,"name":"Spin density waves","url":"https://www.academia.edu/Documents/in/Spin_density_waves?f_ri=34232"},{"id":1958064,"name":"Fermi Surface","url":"https://www.academia.edu/Documents/in/Fermi_Surface?f_ri=34232"},{"id":1958066,"name":"Topological Superconductivity","url":"https://www.academia.edu/Documents/in/Topological_Superconductivity?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_9601545" data-work_id="9601545" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/9601545/An_ARPES_view_on_the_high_T_c_problem_Phonons_vs_spin_fluctuations">An ARPES view on the high-T c problem: Phonons vs. spin-fluctuations</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">We review the search for a mediator of high-Tc superconductivity focusing on ARPES experiment. In case of HTSC cuprates, we summarize and discuss a consistent view of electronic interactions that provides natural explanation of both the... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_9601545" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">We review the search for a mediator of high-Tc superconductivity focusing on ARPES experiment. In case of HTSC cuprates, we summarize and discuss a consistent view of electronic interactions that provides natural explanation of both the origin of the pseudogap state and the mechanism for high temperature superconductivity. Within this scenario, the spin-fluctuations play a decisive role in formation of the fermionic excitation spectrum in the normal state and are sufficient to explain the high transition temperatures to the superconducting state while the pseudogap phenomenon is a consequence of a Peierls-type intrinsic instability of electronic system to formation of an incommensurate density wave. On the other hand, a similar analysis being applied to the iron pnictides reveals especially strong electron-phonon coupling that suggests important role of phonons for high-Tc superconductivity in pnictides.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/9601545" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="00046d5743f01db423b932cd6897b024" rel="nofollow" data-download="{"attachment_id":35809725,"asset_id":9601545,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/35809725/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="22769033" href="https://independent.academia.edu/AlexanderKordyuk">Alexander Kordyuk</a><script data-card-contents-for-user="22769033" type="text/json">{"id":22769033,"first_name":"Alexander","last_name":"Kordyuk","domain_name":"independent","page_name":"AlexanderKordyuk","display_name":"Alexander Kordyuk","profile_url":"https://independent.academia.edu/AlexanderKordyuk?f_ri=34232","photo":"https://gravatar.com/avatar/3f87bce5d32ba67d364010ee6c6fc712?s=65"}</script></span></span></li><li class="js-paper-rank-work_9601545 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="9601545"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 9601545, container: ".js-paper-rank-work_9601545", }); 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$(".js-view-count[data-work-id=9601545]").text(description); $(".js-view-count-work_9601545").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_9601545").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="9601545"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">4</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="6469" rel="nofollow" href="https://www.academia.edu/Documents/in/Superconductivity">Superconductivity</a>, <script data-card-contents-for-ri="6469" type="text/json">{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="32736" rel="nofollow" href="https://www.academia.edu/Documents/in/ARPES">ARPES</a>, <script data-card-contents-for-ri="32736" type="text/json">{"id":32736,"name":"ARPES","url":"https://www.academia.edu/Documents/in/ARPES?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a>, <script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="125513" rel="nofollow" href="https://www.academia.edu/Documents/in/Superconductors">Superconductors</a><script data-card-contents-for-ri="125513" type="text/json">{"id":125513,"name":"Superconductors","url":"https://www.academia.edu/Documents/in/Superconductors?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=9601545]'), work: {"id":9601545,"title":"An ARPES view on the high-T c problem: Phonons vs. spin-fluctuations","created_at":"2014-12-02T16:24:57.480-08:00","url":"https://www.academia.edu/9601545/An_ARPES_view_on_the_high_T_c_problem_Phonons_vs_spin_fluctuations?f_ri=34232","dom_id":"work_9601545","summary":"We review the search for a mediator of high-Tc superconductivity focusing on ARPES experiment. In case of HTSC cuprates, we summarize and discuss a consistent view of electronic interactions that provides natural explanation of both the origin of the pseudogap state and the mechanism for high temperature superconductivity. Within this scenario, the spin-fluctuations play a decisive role in formation of the fermionic excitation spectrum in the normal state and are sufficient to explain the high transition temperatures to the superconducting state while the pseudogap phenomenon is a consequence of a Peierls-type intrinsic instability of electronic system to formation of an incommensurate density wave. On the other hand, a similar analysis being applied to the iron pnictides reveals especially strong electron-phonon coupling that suggests important role of phonons for high-Tc superconductivity in pnictides.","downloadable_attachments":[{"id":35809725,"asset_id":9601545,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":22769033,"first_name":"Alexander","last_name":"Kordyuk","domain_name":"independent","page_name":"AlexanderKordyuk","display_name":"Alexander Kordyuk","profile_url":"https://independent.academia.edu/AlexanderKordyuk?f_ri=34232","photo":"https://gravatar.com/avatar/3f87bce5d32ba67d364010ee6c6fc712?s=65"}],"research_interests":[{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true},{"id":32736,"name":"ARPES","url":"https://www.academia.edu/Documents/in/ARPES?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":125513,"name":"Superconductors","url":"https://www.academia.edu/Documents/in/Superconductors?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_38220072" data-work_id="38220072" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/38220072/Application_of_High_Tc_Superconducting_Josephson_Junction_Devices">Application of High-Tc Superconducting Josephson Junction Devices</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Abstract: The application of superconducting devices based on Josephson junction has been investigated for many years. Josephson junction is based on quantum mechanical tunneling of electrons between weakly coupled two superconducting... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_38220072" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Abstract: The application of superconducting devices based on Josephson junction has been investigated<br />for many years. Josephson junction is based on quantum mechanical tunneling of electrons between weakly <br />coupled two superconducting regions. Its unique properties make it a building block for future <br />superconducting electronic circuits. In this paper, attempt has been made to highlight the wide range of <br />application of Josephson junction including Josephson voltage standard, SQUIDs, Quantum Computer, <br />analog to digital converter, RSFQ digital electronics, terahertz emitter and detector etc.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/38220072" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="630b1e69e33300d8d606c2012ed60c13" rel="nofollow" data-download="{"attachment_id":58259585,"asset_id":38220072,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/58259585/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="39660973" href="https://dbbtcoc.academia.edu/ShailajKumarShrivastava">Shailaj Kumar Shrivastava</a><script data-card-contents-for-user="39660973" type="text/json">{"id":39660973,"first_name":"Shailaj Kumar","last_name":"Shrivastava","domain_name":"dbbtcoc","page_name":"ShailajKumarShrivastava","display_name":"Shailaj Kumar Shrivastava","profile_url":"https://dbbtcoc.academia.edu/ShailajKumarShrivastava?f_ri=34232","photo":"https://0.academia-photos.com/39660973/14421391/158749700/s65_shailaj_kumar.shrivastava.jpg"}</script></span></span></li><li class="js-paper-rank-work_38220072 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="38220072"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 38220072, container: ".js-paper-rank-work_38220072", }); });</script></li><li class="js-percentile-work_38220072 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 38220072; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_38220072"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_38220072 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="38220072"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 38220072; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=38220072]").text(description); $(".js-view-count-work_38220072").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_38220072").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="38220072"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i></div><span class="InlineList-item-text u-textTruncate u-pl6x"><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (false) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=38220072]'), work: {"id":38220072,"title":"Application of High-Tc Superconducting Josephson Junction Devices","created_at":"2019-01-25T07:11:00.383-08:00","url":"https://www.academia.edu/38220072/Application_of_High_Tc_Superconducting_Josephson_Junction_Devices?f_ri=34232","dom_id":"work_38220072","summary":"Abstract: The application of superconducting devices based on Josephson junction has been investigated\nfor many years. Josephson junction is based on quantum mechanical tunneling of electrons between weakly \ncoupled two superconducting regions. Its unique properties make it a building block for future \nsuperconducting electronic circuits. In this paper, attempt has been made to highlight the wide range of \napplication of Josephson junction including Josephson voltage standard, SQUIDs, Quantum Computer, \nanalog to digital converter, RSFQ digital electronics, terahertz emitter and detector etc.","downloadable_attachments":[{"id":58259585,"asset_id":38220072,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":39660973,"first_name":"Shailaj Kumar","last_name":"Shrivastava","domain_name":"dbbtcoc","page_name":"ShailajKumarShrivastava","display_name":"Shailaj Kumar Shrivastava","profile_url":"https://dbbtcoc.academia.edu/ShailajKumarShrivastava?f_ri=34232","photo":"https://0.academia-photos.com/39660973/14421391/158749700/s65_shailaj_kumar.shrivastava.jpg"}],"research_interests":[{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_40419959" data-work_id="40419959" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/40419959/Evolution_of_Pairing_Orders_between_Pseudogap_and_Superconducting_Phases_of_Cuprate_Superconductors">Evolution of Pairing Orders between Pseudogap and Superconducting Phases of Cuprate Superconductors</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">One of the most puzzling problems of high temperature cuprate superconductor is the pseudogap phase (pG) at temperatures above the superconducting transition temperature in the underdoped regime. the pG phase is found by the... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_40419959" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">One of the most puzzling problems of high temperature cuprate superconductor is the pseudogap phase (pG) at temperatures above the superconducting transition temperature in the underdoped regime. the pG phase is found by the angle-resolved photoemission spectra (ARpes) to have a gap at some regions in momentum space and a fraction of Fermi surface remained, known as Fermi arcs. The arc turns into a d-wave SC gap with a node below the SC transition temperature. Here, by studying a strongly correlated model at low temperatures, we obtained a phase characterized by two kinds of pairing order parameters with the total momentum of the Cooper pair to be zero and finite. The finite momentum pairing is accompanied with a spatial modulation of pairing order, i.e. a pair density wave (pDW). these pDW phases are intertwined with modulations of charge density and intra-unit cell form factors. The coexistence of the two different pairing orders provides the unique two-gaps like spectra observed by ARPES for superconducting cuprates. As temperature raises, the zero-momentum pairing order vanishes while the finite momentum pairing orders are kept, thus Fermi arcs are realized. The calculated quasiparticle spectra have the similar doping and temperature dependence as reported by ARPES and scanning tunneling spectroscopy (STS). The consequence of breaking symmetry between x and y due to the unidirectional pDW and the possibility to probe such a pDW state in the pG phase is discussed.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/40419959" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="bf00425e73941fd535d502d6987ce402" rel="nofollow" data-download="{"attachment_id":60675652,"asset_id":40419959,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/60675652/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="18807285" href="https://korea-kr.academia.edu/WeiLinTu">Wei-Lin Tu</a><script data-card-contents-for-user="18807285" type="text/json">{"id":18807285,"first_name":"Wei-Lin","last_name":"Tu","domain_name":"korea-kr","page_name":"WeiLinTu","display_name":"Wei-Lin Tu","profile_url":"https://korea-kr.academia.edu/WeiLinTu?f_ri=34232","photo":"https://0.academia-photos.com/18807285/20579331/20196441/s65_wei-lin.tu.jpg"}</script></span></span></li><li class="js-paper-rank-work_40419959 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="40419959"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 40419959, container: ".js-paper-rank-work_40419959", }); });</script></li><li class="js-percentile-work_40419959 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 40419959; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_40419959"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_40419959 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="40419959"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 40419959; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=40419959]").text(description); $(".js-view-count-work_40419959").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_40419959").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="40419959"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">2</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="505" rel="nofollow" href="https://www.academia.edu/Documents/in/Condensed_Matter_Physics">Condensed Matter Physics</a>, <script data-card-contents-for-ri="505" type="text/json">{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=40419959]'), work: {"id":40419959,"title":"Evolution of Pairing Orders between Pseudogap and Superconducting Phases of Cuprate Superconductors","created_at":"2019-09-23T00:18:26.133-07:00","url":"https://www.academia.edu/40419959/Evolution_of_Pairing_Orders_between_Pseudogap_and_Superconducting_Phases_of_Cuprate_Superconductors?f_ri=34232","dom_id":"work_40419959","summary":"One of the most puzzling problems of high temperature cuprate superconductor is the pseudogap phase (pG) at temperatures above the superconducting transition temperature in the underdoped regime. the pG phase is found by the angle-resolved photoemission spectra (ARpes) to have a gap at some regions in momentum space and a fraction of Fermi surface remained, known as Fermi arcs. The arc turns into a d-wave SC gap with a node below the SC transition temperature. Here, by studying a strongly correlated model at low temperatures, we obtained a phase characterized by two kinds of pairing order parameters with the total momentum of the Cooper pair to be zero and finite. The finite momentum pairing is accompanied with a spatial modulation of pairing order, i.e. a pair density wave (pDW). these pDW phases are intertwined with modulations of charge density and intra-unit cell form factors. The coexistence of the two different pairing orders provides the unique two-gaps like spectra observed by ARPES for superconducting cuprates. As temperature raises, the zero-momentum pairing order vanishes while the finite momentum pairing orders are kept, thus Fermi arcs are realized. The calculated quasiparticle spectra have the similar doping and temperature dependence as reported by ARPES and scanning tunneling spectroscopy (STS). The consequence of breaking symmetry between x and y due to the unidirectional pDW and the possibility to probe such a pDW state in the pG phase is discussed. ","downloadable_attachments":[{"id":60675652,"asset_id":40419959,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":18807285,"first_name":"Wei-Lin","last_name":"Tu","domain_name":"korea-kr","page_name":"WeiLinTu","display_name":"Wei-Lin Tu","profile_url":"https://korea-kr.academia.edu/WeiLinTu?f_ri=34232","photo":"https://0.academia-photos.com/18807285/20579331/20196441/s65_wei-lin.tu.jpg"}],"research_interests":[{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_28094938" data-work_id="28094938" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/28094938/Scale_free_structural_organization_of_oxygen_interstitials_in_La2CuO4_y">Scale-free structural organization of oxygen interstitials in La2CuO4+y</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">It is well known that the microstructures of the transition-metal oxides 1-3 , including the high-transition-temperature (high-T c ) copper oxide superconductors 4-7 , are complex. This is particularly so when there are oxygen... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_28094938" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">It is well known that the microstructures of the transition-metal oxides 1-3 , including the high-transition-temperature (high-T c ) copper oxide superconductors 4-7 , are complex. This is particularly so when there are oxygen interstitials or vacancies 8 , which influence the bulk properties. For example, the oxygen interstitials in the spacer layers separating the superconducting CuO 2 planes undergo ordering phenomena in Sr 2 O 11y CuO 2 (ref. 9), YBa 2 Cu 3 O 61y (ref. 10) and La 2 CuO 41y (refs 11-15) that induce enhancements in the transition temperatures with no changes in hole concentrations. It is also known that complex systems often have a scale-invariant structural organization 16 , but hitherto none had been found in high-T c materials. Here we report that the ordering of oxygen interstitials in the La 2 O 21y spacer layers of La 2 CuO 41y high-T c superconductors is characterized by a fractal distribution up to a maximum limiting size of 400 mm. Intriguingly, these fractal distributions of dopants seem to enhance superconductivity at high temperature.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/28094938" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="824aa9e29cecd0ecbc550080b400bfac" rel="nofollow" data-download="{"attachment_id":48410066,"asset_id":28094938,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/48410066/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="52657221" href="https://independent.academia.edu/FratiniM">M. 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This is particularly so when there are oxygen interstitials or vacancies 8 , which influence the bulk properties. For example, the oxygen interstitials in the spacer layers separating the superconducting CuO 2 planes undergo ordering phenomena in Sr 2 O 11y CuO 2 (ref. 9), YBa 2 Cu 3 O 61y (ref. 10) and La 2 CuO 41y (refs 11-15) that induce enhancements in the transition temperatures with no changes in hole concentrations. It is also known that complex systems often have a scale-invariant structural organization 16 , but hitherto none had been found in high-T c materials. Here we report that the ordering of oxygen interstitials in the La 2 O 21y spacer layers of La 2 CuO 41y high-T c superconductors is characterized by a fractal distribution up to a maximum limiting size of 400 mm. Intriguingly, these fractal distributions of dopants seem to enhance superconductivity at high temperature.","downloadable_attachments":[{"id":48410066,"asset_id":28094938,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":52657221,"first_name":"M.","last_name":"Fratini","domain_name":"independent","page_name":"FratiniM","display_name":"M. 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Analysis","url":"https://www.academia.edu/Documents/in/Statistical_Analysis?f_ri=34232"},{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232"},{"id":11973,"name":"Nanomaterials","url":"https://www.academia.edu/Documents/in/Nanomaterials?f_ri=34232"},{"id":16460,"name":"Statistical Physics","url":"https://www.academia.edu/Documents/in/Statistical_Physics?f_ri=34232"},{"id":21565,"name":"Statistical Physics Of Complex Systems","url":"https://www.academia.edu/Documents/in/Statistical_Physics_Of_Complex_Systems?f_ri=34232"},{"id":24831,"name":"Fractals","url":"https://www.academia.edu/Documents/in/Fractals?f_ri=34232"},{"id":25035,"name":"Material Science","url":"https://www.academia.edu/Documents/in/Material_Science?f_ri=34232"},{"id":28235,"name":"Multidisciplinary","url":"https://www.academia.edu/Documents/in/Multidisciplinary?f_ri=34232"},{"id":32745,"name":"Strongly-correlated electron 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u-mb0x js-work-card work_12896844 coauthored" data-work_id="12896844" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/12896844/The_Microstrain_Doping_Phase_Diagram_of_the_Iron_Pnictides_Heterostructures_at_Atomic_Limit">The Microstrain-Doping Phase Diagram of the Iron Pnictides: Heterostructures at Atomic Limit</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">The 3D phase diagram of iron pnictides where the critical temperature depends on charge density and microstrain in the active FeAs layers is proposed. The iron pnictides superconductors are shown to be a practical realization of a... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_12896844" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">The 3D phase diagram of iron pnictides where the critical temperature depends on charge density and microstrain in the active FeAs layers is proposed. The iron pnictides superconductors are shown to be a practical realization of a heterostructure at the atomic limit made of a superlattice of FeAs layers intercalated by spacers layers. We have focussed our interest on the A 1-x B x Fe 2 As 2 (122) families and we show that FeAs layers have a tensile microstrain due to the misfit strain between the active layers and the spacers. We have identified the critical range of doping and microstrain where the critical temperature gets amplified to its maximum value.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/12896844" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="6e7abd17da796dd86b75dc245123fa10" rel="nofollow" data-download="{"attachment_id":45860988,"asset_id":12896844,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/45860988/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="33288630" href="https://wwwuniroma1.academia.edu/ABianconi">A. Bianconi</a><script data-card-contents-for-user="33288630" type="text/json">{"id":33288630,"first_name":"A.","last_name":"Bianconi","domain_name":"wwwuniroma1","page_name":"ABianconi","display_name":"A. Bianconi","profile_url":"https://wwwuniroma1.academia.edu/ABianconi?f_ri=34232","photo":"/images/s65_no_pic.png"}</script></span></span><span class="u-displayInlineBlock InlineList-item-text"> and <span class="u-textDecorationUnderline u-clickable InlineList-item-text js-work-more-authors-12896844">+1</span><div class="hidden js-additional-users-12896844"><div><span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a href="https://unicatt.academia.edu/GabrieleCiasca">Gabriele Ciasca</a></span></div></div></span><script>(function(){ var popoverSettings = { el: $('.js-work-more-authors-12896844'), placement: 'bottom', hide_delay: 200, html: true, content: function(){ return $('.js-additional-users-12896844').html(); } } new HoverPopover(popoverSettings); })();</script></li><li class="js-paper-rank-work_12896844 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="12896844"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 12896844, container: ".js-paper-rank-work_12896844", }); });</script></li><li class="js-percentile-work_12896844 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 12896844; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_12896844"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_12896844 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="12896844"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 12896844; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=12896844]").text(description); $(".js-view-count-work_12896844").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_12896844").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="12896844"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">18</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="505" rel="nofollow" href="https://www.academia.edu/Documents/in/Condensed_Matter_Physics">Condensed Matter Physics</a>, <script data-card-contents-for-ri="505" type="text/json">{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="6469" rel="nofollow" href="https://www.academia.edu/Documents/in/Superconductivity">Superconductivity</a>, <script data-card-contents-for-ri="6469" type="text/json">{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="33912" rel="nofollow" href="https://www.academia.edu/Documents/in/Doping">Doping</a>, <script data-card-contents-for-ri="33912" type="text/json">{"id":33912,"name":"Doping","url":"https://www.academia.edu/Documents/in/Doping?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=12896844]'), work: {"id":12896844,"title":"The Microstrain-Doping Phase Diagram of the Iron Pnictides: Heterostructures at Atomic Limit","created_at":"2015-06-10T00:27:49.584-07:00","url":"https://www.academia.edu/12896844/The_Microstrain_Doping_Phase_Diagram_of_the_Iron_Pnictides_Heterostructures_at_Atomic_Limit?f_ri=34232","dom_id":"work_12896844","summary":"The 3D phase diagram of iron pnictides where the critical temperature depends on charge density and microstrain in the active FeAs layers is proposed. The iron pnictides superconductors are shown to be a practical realization of a heterostructure at the atomic limit made of a superlattice of FeAs layers intercalated by spacers layers. We have focussed our interest on the A 1-x B x Fe 2 As 2 (122) families and we show that FeAs layers have a tensile microstrain due to the misfit strain between the active layers and the spacers. We have identified the critical range of doping and microstrain where the critical temperature gets amplified to its maximum value.","downloadable_attachments":[{"id":45860988,"asset_id":12896844,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":33288630,"first_name":"A.","last_name":"Bianconi","domain_name":"wwwuniroma1","page_name":"ABianconi","display_name":"A. Bianconi","profile_url":"https://wwwuniroma1.academia.edu/ABianconi?f_ri=34232","photo":"/images/s65_no_pic.png"},{"id":32052246,"first_name":"Gabriele","last_name":"Ciasca","domain_name":"unicatt","page_name":"GabrieleCiasca","display_name":"Gabriele Ciasca","profile_url":"https://unicatt.academia.edu/GabrieleCiasca?f_ri=34232","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics?f_ri=34232","nofollow":true},{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true},{"id":33912,"name":"Doping","url":"https://www.academia.edu/Documents/in/Doping?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":50630,"name":"Crystal structure","url":"https://www.academia.edu/Documents/in/Crystal_structure?f_ri=34232"},{"id":59221,"name":"Phase Diagrams","url":"https://www.academia.edu/Documents/in/Phase_Diagrams?f_ri=34232"},{"id":125513,"name":"Superconductors","url":"https://www.academia.edu/Documents/in/Superconductors?f_ri=34232"},{"id":158597,"name":"Iron","url":"https://www.academia.edu/Documents/in/Iron?f_ri=34232"},{"id":179365,"name":"Cuprates","url":"https://www.academia.edu/Documents/in/Cuprates?f_ri=34232"},{"id":414312,"name":"Strain","url":"https://www.academia.edu/Documents/in/Strain?f_ri=34232"},{"id":527291,"name":"Microstrain","url":"https://www.academia.edu/Documents/in/Microstrain?f_ri=34232"},{"id":772730,"name":"Charge Density","url":"https://www.academia.edu/Documents/in/Charge_Density?f_ri=34232"},{"id":961390,"name":"Superstructure","url":"https://www.academia.edu/Documents/in/Superstructure?f_ri=34232"},{"id":1130298,"name":"Critical Point","url":"https://www.academia.edu/Documents/in/Critical_Point?f_ri=34232"},{"id":1154530,"name":"Tensile Stress","url":"https://www.academia.edu/Documents/in/Tensile_Stress?f_ri=34232"},{"id":1207994,"name":"High Tc Superconductivity","url":"https://www.academia.edu/Documents/in/High_Tc_Superconductivity?f_ri=34232"},{"id":1337673,"name":"Active Layer","url":"https://www.academia.edu/Documents/in/Active_Layer?f_ri=34232"},{"id":1371366,"name":"Superlattices","url":"https://www.academia.edu/Documents/in/Superlattices?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_8795423" data-work_id="8795423" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/8795423/MANAGING_AND_EVALUATING_THE_IMPACTS_OF_LARGE_RESEARCH_PROGRAMMES">MANAGING AND EVALUATING THE IMPACTS OF LARGE RESEARCH PROGRAMMES</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">This research was funded by, and implemented within, a UK national research organisation, while the author was the KE and Impact Evaluation Manager responsible for assessing impact on a £15m UK government-funded research programme. This... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_8795423" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">This research was funded by, and implemented within, a UK national research organisation, while the author was the KE and Impact Evaluation Manager responsible for assessing impact on a £15m UK government-funded research programme.<br /><br />This work was also submitted as the authors MBA dissertation which was accepted and awarded in 2009. <br /><br />ABSTRACT: A methodology and methods ‘toolbox’ is proposed for conducting impact research and assessment from within research programmes. The emphasis is upon how to clarify and assess the wider impacts from the early stages onwards.<br /><br />The approach explicitly acknowledges, and attempts to address, the known issues and challenges of impact assessment while drawing upon the resources and opportunities available to research managers and researchers within such programmes.<br /><br />The study has two triangulating foundations. Firstly, it examines the academic literature to help identify and design the pilot methodology and methods. Secondly it trials these in a real programme to both test and improve them.<br /><br />The study was conducted over one year within one leading UK research organisation, where two research programmes (and around 60 research projects of £15m total value) were being assessed for their impacts. The study draws upon actual impact management experience and reflection, prospective (ex ante) and retrospective (ex post) assessments, participatory contributions from leading researchers undergoing assessment, and consultation with external users. The findings of this study outline the pilot and its first iteration. Recommendations are made for improvement to the methodology and methods.<br /><br />A subsequent follow-on bid to UK government incorporating the impacts identified from implementing this methodology, successfully led to a further £15m of government funding.<br /><br />It is expected the pilot methodology and methods will be applicable to other organisations, conducting and funding such research programmes, required to research and assess the wider research impacts. <br /><br />Although primary focus of implemetation trials was upon research in physical sciences, technology, high-tech engineering, computing/IT, and environment, the wider literature study, the methodology design and justification, the methods proposed and used, and the resulting general recommendations and lessons are expected to apply more broadly to many other research areas, where the impact is to be found more widely in the society, economy, government or public sector or within organizations, policies, professions or the public.<br /><br />Interest in this work is expected from research programme managers, impact managers and assessors, management consultants advising in this area, and government funding managers, all seeking to embed a developing approach to understand, capture, and enhance wider impact.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/8795423" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="3ad5b3758f02334aa03f3f803fce403e" rel="nofollow" data-download="{"attachment_id":35457082,"asset_id":8795423,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/35457082/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="18878088" href="https://independent.academia.edu/trevorwren">Trevor Wren BSc MA MPhil PhD MBA</a><script data-card-contents-for-user="18878088" type="text/json">{"id":18878088,"first_name":"Trevor","last_name":"Wren BSc MA MPhil PhD MBA","domain_name":"independent","page_name":"trevorwren","display_name":"Trevor Wren BSc MA MPhil PhD MBA","profile_url":"https://independent.academia.edu/trevorwren?f_ri=34232","photo":"https://0.academia-photos.com/18878088/5247911/6001811/s65_trevor.wren.jpg_oh_12adb13cb0c446279d6b0139cd929fbc_oe_54f03f51___gda___1425507246_85468fc3920de1b4fce8638dfb1ba988"}</script></span></span></li><li class="js-paper-rank-work_8795423 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="8795423"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 8795423, container: ".js-paper-rank-work_8795423", }); 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$(".js-view-count[data-work-id=8795423]").text(description); $(".js-view-count-work_8795423").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_8795423").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="8795423"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">1018</a>  </div><span class="InlineList-item-text u-textTruncate u-pl12x"><a class="InlineList-item-text" data-has-card-for-ri="38" rel="nofollow" href="https://www.academia.edu/Documents/in/Management">Management</a>, <script data-card-contents-for-ri="38" type="text/json">{"id":38,"name":"Management","url":"https://www.academia.edu/Documents/in/Management?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="45" rel="nofollow" href="https://www.academia.edu/Documents/in/Business_Administration">Business Administration</a>, <script data-card-contents-for-ri="45" type="text/json">{"id":45,"name":"Business Administration","url":"https://www.academia.edu/Documents/in/Business_Administration?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="48" rel="nofollow" href="https://www.academia.edu/Documents/in/Engineering">Engineering</a>, <script data-card-contents-for-ri="48" type="text/json">{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="49" rel="nofollow" href="https://www.academia.edu/Documents/in/Electrical_Engineering">Electrical Engineering</a><script data-card-contents-for-ri="49" type="text/json">{"id":49,"name":"Electrical Engineering","url":"https://www.academia.edu/Documents/in/Electrical_Engineering?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=8795423]'), work: {"id":8795423,"title":"MANAGING AND EVALUATING THE IMPACTS OF LARGE RESEARCH PROGRAMMES","created_at":"2014-10-15T07:15:10.553-07:00","url":"https://www.academia.edu/8795423/MANAGING_AND_EVALUATING_THE_IMPACTS_OF_LARGE_RESEARCH_PROGRAMMES?f_ri=34232","dom_id":"work_8795423","summary":"This research was funded by, and implemented within, a UK national research organisation, while the author was the KE and Impact Evaluation Manager responsible for assessing impact on a £15m UK government-funded research programme.\n\nThis work was also submitted as the authors MBA dissertation which was accepted and awarded in 2009. \n\nABSTRACT: A methodology and methods ‘toolbox’ is proposed for conducting impact research and assessment from within research programmes. The emphasis is upon how to clarify and assess the wider impacts from the early stages onwards.\n\nThe approach explicitly acknowledges, and attempts to address, the known issues and challenges of impact assessment while drawing upon the resources and opportunities available to research managers and researchers within such programmes.\n\nThe study has two triangulating foundations. Firstly, it examines the academic literature to help identify and design the pilot methodology and methods. Secondly it trials these in a real programme to both test and improve them.\n\nThe study was conducted over one year within one leading UK research organisation, where two research programmes (and around 60 research projects of £15m total value) were being assessed for their impacts. The study draws upon actual impact management experience and reflection, prospective (ex ante) and retrospective (ex post) assessments, participatory contributions from leading researchers undergoing assessment, and consultation with external users. The findings of this study outline the pilot and its first iteration. Recommendations are made for improvement to the methodology and methods.\n\nA subsequent follow-on bid to UK government incorporating the impacts identified from implementing this methodology, successfully led to a further £15m of government funding.\n\nIt is expected the pilot methodology and methods will be applicable to other organisations, conducting and funding such research programmes, required to research and assess the wider research impacts. \n\nAlthough primary focus of implemetation trials was upon research in physical sciences, technology, high-tech engineering, computing/IT, and environment, the wider literature study, the methodology design and justification, the methods proposed and used, and the resulting general recommendations and lessons are expected to apply more broadly to many other research areas, where the impact is to be found more widely in the society, economy, government or public sector or within organizations, policies, professions or the public.\n\nInterest in this work is expected from research programme managers, impact managers and assessors, management consultants advising in this area, and government funding managers, all seeking to embed a developing approach to understand, capture, and enhance wider impact. 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})();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_38966069 coauthored" data-work_id="38966069" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/38966069/REGRESSION_OF_SUPERCONDUCTING_CRITICAL_TEMPERATURE_USING_A_PCA_GRID_SEARCH_ADA_BOOST_REGRESSION_MODEL">REGRESSION OF SUPERCONDUCTING CRITICAL TEMPERATURE: USING A PCA-GRID SEARCH-ADA BOOST REGRESSION MODEL</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Superconductivity is being studied since its discovery more than a century ago. The numerous applications of the superconductors made it a subject of intense research. Despite being studied for so long, some of its properties remain a... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_38966069" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Superconductivity is being studied since its discovery more than a century ago. The numerous applications of the superconductors made it a subject of intense research. Despite being studied for so long, some of its properties remain a mystery. One of the interesting properties of a super conductor is its critical temperature. Superconductors exhibit zero electrical resistance when maintained at the critical temperature. The value of critical temperature is different for each superconducting material. This value is experimentally calculated by measuring resistance against the temperature of the material. In this project, by taking advantage of the immense increase of readily accessible and potentially relevant information, we develop several machine learning methods modeling critical temperature of a super conductor based on its chemical properties. The final model will give an estimate of critical temperature of a superconductor. This estimate provides confidence on a newly discovered material to continue further research on it.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/38966069" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="b6cf8c4947579248443850c56969c4a2" rel="nofollow" data-download="{"attachment_id":59069826,"asset_id":38966069,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/59069826/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="13733577" rel="nofollow" href="https://iiitb.academia.edu/IJIRAEInternationalJournalofInnovativeResearchinAdvancedEngineering">IJIRAE - International Journal of Innovative Research in Advanced Engineering</a><script data-card-contents-for-user="13733577" type="text/json">{"id":13733577,"first_name":"IJIRAE","last_name":"International Journal of Innovative Research in Advanced Engineering","domain_name":"iiitb","page_name":"IJIRAEInternationalJournalofInnovativeResearchinAdvancedEngineering","display_name":"IJIRAE - International Journal of Innovative Research in Advanced Engineering","profile_url":"https://iiitb.academia.edu/IJIRAEInternationalJournalofInnovativeResearchinAdvancedEngineering?f_ri=34232","photo":"https://0.academia-photos.com/13733577/3819053/35118444/s65_ijirae.international_journal_of_innovative_research_in_advanced_engineering.jpg"}</script></span></span><span class="u-displayInlineBlock InlineList-item-text"> and <span class="u-textDecorationUnderline u-clickable InlineList-item-text js-work-more-authors-38966069">+1</span><div class="hidden js-additional-users-38966069"><div><span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a href="https://independent.academia.edu/SureshParachuri">Suresh Parachuri</a></span></div></div></span><script>(function(){ var popoverSettings = { el: $('.js-work-more-authors-38966069'), placement: 'bottom', hide_delay: 200, html: true, content: function(){ return $('.js-additional-users-38966069').html(); 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The numerous applications of the superconductors made it a subject of intense research. Despite being studied for so long, some of its properties remain a mystery. One of the interesting properties of a super conductor is its critical temperature. Superconductors exhibit zero electrical resistance when maintained at the critical temperature. The value of critical temperature is different for each superconducting material. This value is experimentally calculated by measuring resistance against the temperature of the material. In this project, by taking advantage of the immense increase of readily accessible and potentially relevant information, we develop several machine learning methods modeling critical temperature of a super conductor based on its chemical properties. The final model will give an estimate of critical temperature of a superconductor. This estimate provides confidence on a newly discovered material to continue further research on it.","downloadable_attachments":[{"id":59069826,"asset_id":38966069,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":13733577,"first_name":"IJIRAE","last_name":"International Journal of Innovative Research in Advanced Engineering","domain_name":"iiitb","page_name":"IJIRAEInternationalJournalofInnovativeResearchinAdvancedEngineering","display_name":"IJIRAE - International Journal of Innovative Research in Advanced Engineering","profile_url":"https://iiitb.academia.edu/IJIRAEInternationalJournalofInnovativeResearchinAdvancedEngineering?f_ri=34232","photo":"https://0.academia-photos.com/13733577/3819053/35118444/s65_ijirae.international_journal_of_innovative_research_in_advanced_engineering.jpg"},{"id":111964910,"first_name":"Suresh","last_name":"Parachuri","domain_name":"independent","page_name":"SureshParachuri","display_name":"Suresh Parachuri","profile_url":"https://independent.academia.edu/SureshParachuri?f_ri=34232","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":2008,"name":"Machine Learning","url":"https://www.academia.edu/Documents/in/Machine_Learning?f_ri=34232","nofollow":true},{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":53338,"name":"Decision Trees","url":"https://www.academia.edu/Documents/in/Decision_Trees?f_ri=34232","nofollow":true},{"id":70938,"name":"Electrical Power Systems,renewable Energy Sources, Applied Superconductivity","url":"https://www.academia.edu/Documents/in/Electrical_Power_Systems_renewable_Energy_Sources_Applied_Superconductivity?f_ri=34232"},{"id":70942,"name":"Electric Power Applications of Superconductivity","url":"https://www.academia.edu/Documents/in/Electric_Power_Applications_of_Superconductivity?f_ri=34232"},{"id":107672,"name":"Regression","url":"https://www.academia.edu/Documents/in/Regression?f_ri=34232"},{"id":123230,"name":"Regression Analysis","url":"https://www.academia.edu/Documents/in/Regression_Analysis?f_ri=34232"},{"id":134046,"name":"Electron transport in novel graphene based nano-structures, topological Insulators, superconductivity in nanoscale systems.","url":"https://www.academia.edu/Documents/in/Electron_transport_in_novel_graphene_based_nano-structures_topological_Insulators_superconductivit?f_ri=34232"},{"id":175871,"name":"AdaBoost","url":"https://www.academia.edu/Documents/in/AdaBoost?f_ri=34232"},{"id":669819,"name":"Extreme Learning Machines","url":"https://www.academia.edu/Documents/in/Extreme_Learning_Machines?f_ri=34232"},{"id":986283,"name":"Cognitive Models of Human Learning","url":"https://www.academia.edu/Documents/in/Cognitive_Models_of_Human_Learning?f_ri=34232"},{"id":1117034,"name":"Applied Superconductivity Fault Current Limiter","url":"https://www.academia.edu/Documents/in/Applied_Superconductivity_Fault_Current_Limiter?f_ri=34232"},{"id":1379644,"name":"AdaBoost Algorithm","url":"https://www.academia.edu/Documents/in/AdaBoost_Algorithm?f_ri=34232"},{"id":1394433,"name":"Critical Temperature","url":"https://www.academia.edu/Documents/in/Critical_Temperature?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_55794037" data-work_id="55794037" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/55794037/Modelling_of_bulk_superconductor_magnetization">Modelling of bulk superconductor magnetization</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">This paper presents a topical review of the current state of the art in modelling the magnetization of bulk superconductors, including both (RE)BCO (where RE = rare earth or Y) and MgB2 materials. Such modelling is a powerful tool to... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_55794037" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">This paper presents a topical review of the current state of the art in modelling the magnetization of bulk superconductors, including both (RE)BCO (where RE = rare earth or Y) and MgB2 materials. Such modelling is a powerful tool to understand the physical mechanisms of their magnetization, to assist in interpretation of experimental results, and to predict the performance of practical bulk superconductor-based devices, which is particularly important as many superconducting applications head towards the commercialization stage of their development in the coming years. In addition to the analytical and numerical techniques currently used by researchers for modelling such materials, the commonly used practical techniques to magnetize bulk superconductors are summarized with a particular focus on pulsed field magnetization (PFM), which is promising as a compact, mobile and relatively inexpensive magnetizing technique. A number of numerical models developed to analyse the issues relat...</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/55794037" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="151eab68752a4760c490f9a15fbf9168" rel="nofollow" data-download="{"attachment_id":71496505,"asset_id":55794037,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/71496505/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="47601837" href="https://independent.academia.edu/HFujishiro">H. 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Such modelling is a powerful tool to understand the physical mechanisms of their magnetization, to assist in interpretation of experimental results, and to predict the performance of practical bulk superconductor-based devices, which is particularly important as many superconducting applications head towards the commercialization stage of their development in the coming years. In addition to the analytical and numerical techniques currently used by researchers for modelling such materials, the commonly used practical techniques to magnetize bulk superconductors are summarized with a particular focus on pulsed field magnetization (PFM), which is promising as a compact, mobile and relatively inexpensive magnetizing technique. A number of numerical models developed to analyse the issues relat...","downloadable_attachments":[{"id":71496505,"asset_id":55794037,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":47601837,"first_name":"H.","last_name":"Fujishiro","domain_name":"independent","page_name":"HFujishiro","display_name":"H. 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The tribological performance of biodiesel is crucial for its application in automobiles. In the present study, effect of... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_2373151" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Biodiesel, as an alternative fuel is steadily gaining attention to replace petroleum diesel partially or completely. The tribological performance of biodiesel is crucial for its application in automobiles. In the present study, effect of temperature on the tribological performance of palm biodiesel was investigated by using four ball wear machine. Tests were conducted at temperatures 30, 45, 60 and 75 °C, under a normal load of 40 kg for 1 h at speed 1200 rpm. For each temperature, the tribological properties of petroleum diesel (B0) and three biodiesel blends like B10, B20, B50 were investigated and compared. During the wear test, frictional torque was recorded on line. Wear scars in tested ball were investigated by optical microscopy. Results show that friction and wear increase with increasing temperature. <br /> <br /><a href="http://www.sciencedirect.com/science/article/pii/S0360544209005210%5C" rel="nofollow">http://www.sciencedirect.com/science/article/pii/S0360544209005210%5C</a></div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/2373151" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="8408423b4401371209236608ee3550b5" rel="nofollow" data-download="{"attachment_id":31587482,"asset_id":2373151,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/31587482/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="3054445" href="https://malaya.academia.edu/HaseebASMA">Haseeb ASMA</a><script data-card-contents-for-user="3054445" type="text/json">{"id":3054445,"first_name":"Haseeb","last_name":"ASMA","domain_name":"malaya","page_name":"HaseebASMA","display_name":"Haseeb ASMA","profile_url":"https://malaya.academia.edu/HaseebASMA?f_ri=34232","photo":"https://0.academia-photos.com/3054445/1004285/1255894/s65_haseeb.asma.jpg"}</script></span></span></li><li class="js-paper-rank-work_2373151 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="2373151"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 2373151, container: ".js-paper-rank-work_2373151", }); 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The tribological performance of biodiesel is crucial for its application in automobiles. In the present study, effect of temperature on the tribological performance of palm biodiesel was investigated by using four ball wear machine. Tests were conducted at temperatures 30, 45, 60 and 75 °C, under a normal load of 40 kg for 1 h at speed 1200 rpm. For each temperature, the tribological properties of petroleum diesel (B0) and three biodiesel blends like B10, B20, B50 were investigated and compared. During the wear test, frictional torque was recorded on line. Wear scars in tested ball were investigated by optical microscopy. Results show that friction and wear increase with increasing temperature.\r\n\r\nhttp://www.sciencedirect.com/science/article/pii/S0360544209005210%5C ","downloadable_attachments":[{"id":31587482,"asset_id":2373151,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":3054445,"first_name":"Haseeb","last_name":"ASMA","domain_name":"malaya","page_name":"HaseebASMA","display_name":"Haseeb ASMA","profile_url":"https://malaya.academia.edu/HaseebASMA?f_ri=34232","photo":"https://0.academia-photos.com/3054445/1004285/1255894/s65_haseeb.asma.jpg"}],"research_interests":[{"id":48,"name":"Engineering","url":"https://www.academia.edu/Documents/in/Engineering?f_ri=34232","nofollow":true},{"id":55,"name":"Environmental Engineering","url":"https://www.academia.edu/Documents/in/Environmental_Engineering?f_ri=34232","nofollow":true},{"id":72,"name":"Chemical 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Fuel","url":"https://www.academia.edu/Documents/in/Alternative_Fuel?f_ri=34232"},{"id":218344,"name":"Effects of Temperature on the Compressive Strength of a Concrete","url":"https://www.academia.edu/Documents/in/Effects_of_Temperature_on_the_Compressive_Strength_of_a_Concrete?f_ri=34232"},{"id":226548,"name":"Opportunity Gap","url":"https://www.academia.edu/Documents/in/Opportunity_Gap?f_ri=34232"},{"id":262885,"name":"Fish Physiology Effect of Temperature","url":"https://www.academia.edu/Documents/in/Fish_Physiology_Effect_of_Temperature?f_ri=34232"},{"id":377915,"name":"Bioprocessing","url":"https://www.academia.edu/Documents/in/Bioprocessing?f_ri=34232"},{"id":497167,"name":"Friction and wear","url":"https://www.academia.edu/Documents/in/Friction_and_wear?f_ri=34232"},{"id":753627,"name":"Wear Test","url":"https://www.academia.edu/Documents/in/Wear_Test?f_ri=34232"},{"id":828946,"name":"Comparative assessment of injection, combustion, performance and emission characteristics of a diesel engine for biodiesel-diesel blends","url":"https://www.academia.edu/Documents/in/Comparative_assessment_of_injection_combustion_performance_and_emission_characteristics_of_a_diese?f_ri=34232"},{"id":850801,"name":"Tribological Properties","url":"https://www.academia.edu/Documents/in/Tribological_Properties?f_ri=34232"},{"id":902611,"name":"Lubricity","url":"https://www.academia.edu/Documents/in/Lubricity?f_ri=34232"},{"id":902613,"name":"Frictional Torque","url":"https://www.academia.edu/Documents/in/Frictional_Torque?f_ri=34232"},{"id":902614,"name":"Normal Loads","url":"https://www.academia.edu/Documents/in/Normal_Loads?f_ri=34232"},{"id":902623,"name":"Petroleum Diesel","url":"https://www.academia.edu/Documents/in/Petroleum_Diesel?f_ri=34232"},{"id":902624,"name":"Tribological Performance","url":"https://www.academia.edu/Documents/in/Tribological_Performance?f_ri=34232"},{"id":931644,"name":"Bioproducts","url":"https://www.academia.edu/Documents/in/Bioproducts?f_ri=34232"},{"id":931645,"name":"Biomass Processing","url":"https://www.academia.edu/Documents/in/Biomass_Processing?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_19267532" data-work_id="19267532" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/19267532/Theory_of_Plastic_Vortex_Creep">Theory of Plastic Vortex Creep</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">We develop a theory for plastic vortex creep in a topologically disordered (dislocated) vortex solid phase in type-II superconductors in terms of driven thermally activated dislocation dynamics. Plastic barriers for dislocations show a... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_19267532" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">We develop a theory for plastic vortex creep in a topologically disordered (dislocated) vortex solid phase in type-II superconductors in terms of driven thermally activated dislocation dynamics. Plastic barriers for dislocations show a power-law divergence at small driving currents j, U pl ͑ j͒~j 2m , with m 1 for a single dislocation and m 2͞5 for creep of dislocation bundles. This implies a suppression of the creep rate at the transition from the ordered vortex phase (m 2͞11) to the dislocated glass and can manifest itself as an observed increase of the apparent critical current (second peak). Our approach applies to general dynamics of disordered elastic media on a random substrate.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/19267532" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="49f3b4ba265815c6214e89b97f053a04" rel="nofollow" data-download="{"attachment_id":40526084,"asset_id":19267532,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/40526084/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="39369229" href="https://ost-ch.academia.edu/HenrikNordborg">Henrik Nordborg</a><script data-card-contents-for-user="39369229" type="text/json">{"id":39369229,"first_name":"Henrik","last_name":"Nordborg","domain_name":"ost-ch","page_name":"HenrikNordborg","display_name":"Henrik Nordborg","profile_url":"https://ost-ch.academia.edu/HenrikNordborg?f_ri=34232","photo":"https://0.academia-photos.com/39369229/11171103/12466072/s65_henrik.nordborg.jpg"}</script></span></span></li><li class="js-paper-rank-work_19267532 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="19267532"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 19267532, container: ".js-paper-rank-work_19267532", }); });</script></li><li class="js-percentile-work_19267532 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 19267532; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_19267532"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_19267532 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="19267532"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 19267532; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=19267532]").text(description); $(".js-view-count-work_19267532").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_19267532").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="19267532"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">10</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="505" rel="nofollow" href="https://www.academia.edu/Documents/in/Condensed_Matter_Physics">Condensed Matter Physics</a>, <script data-card-contents-for-ri="505" type="text/json">{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="6469" rel="nofollow" href="https://www.academia.edu/Documents/in/Superconductivity">Superconductivity</a>, <script data-card-contents-for-ri="6469" type="text/json">{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a>, <script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="98927" rel="nofollow" href="https://www.academia.edu/Documents/in/Crystal_Plasticity">Crystal Plasticity</a><script data-card-contents-for-ri="98927" type="text/json">{"id":98927,"name":"Crystal Plasticity","url":"https://www.academia.edu/Documents/in/Crystal_Plasticity?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=19267532]'), work: {"id":19267532,"title":"Theory of Plastic Vortex Creep","created_at":"2015-11-30T22:19:47.534-08:00","url":"https://www.academia.edu/19267532/Theory_of_Plastic_Vortex_Creep?f_ri=34232","dom_id":"work_19267532","summary":"We develop a theory for plastic vortex creep in a topologically disordered (dislocated) vortex solid phase in type-II superconductors in terms of driven thermally activated dislocation dynamics. Plastic barriers for dislocations show a power-law divergence at small driving currents j, U pl ͑ j͒~j 2m , with m 1 for a single dislocation and m 2͞5 for creep of dislocation bundles. This implies a suppression of the creep rate at the transition from the ordered vortex phase (m 2͞11) to the dislocated glass and can manifest itself as an observed increase of the apparent critical current (second peak). Our approach applies to general dynamics of disordered elastic media on a random substrate.","downloadable_attachments":[{"id":40526084,"asset_id":19267532,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":39369229,"first_name":"Henrik","last_name":"Nordborg","domain_name":"ost-ch","page_name":"HenrikNordborg","display_name":"Henrik Nordborg","profile_url":"https://ost-ch.academia.edu/HenrikNordborg?f_ri=34232","photo":"https://0.academia-photos.com/39369229/11171103/12466072/s65_henrik.nordborg.jpg"}],"research_interests":[{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics?f_ri=34232","nofollow":true},{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":98927,"name":"Crystal Plasticity","url":"https://www.academia.edu/Documents/in/Crystal_Plasticity?f_ri=34232","nofollow":true},{"id":113890,"name":"Power Law","url":"https://www.academia.edu/Documents/in/Power_Law?f_ri=34232"},{"id":118582,"name":"Physical sciences","url":"https://www.academia.edu/Documents/in/Physical_sciences?f_ri=34232"},{"id":125513,"name":"Superconductors","url":"https://www.academia.edu/Documents/in/Superconductors?f_ri=34232"},{"id":152679,"name":"Dislocations","url":"https://www.academia.edu/Documents/in/Dislocations?f_ri=34232"},{"id":745537,"name":"Thermal Activation","url":"https://www.academia.edu/Documents/in/Thermal_Activation?f_ri=34232"},{"id":769964,"name":"Dislocation dynamics","url":"https://www.academia.edu/Documents/in/Dislocation_dynamics?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_1174603" data-work_id="1174603" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/1174603/Modeling_the_dielectric_behaviors_of_perovskites_ferroelectrics_and_incipient_ferroelectrics">Modeling the dielectric behaviors of perovskites : ferroelectrics and incipient ferroelectrics</a></div></div><div class="u-pb4x u-mt3x"></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/1174603" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="080a2357826e1a70484a97f154d255c8" rel="nofollow" data-download="{"attachment_id":21734197,"asset_id":1174603,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/21734197/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="100272" href="https://manchester.academia.edu/HaiYaoDENG">Hai-Yao DENG</a><script data-card-contents-for-user="100272" type="text/json">{"id":100272,"first_name":"Hai-Yao","last_name":"DENG","domain_name":"manchester","page_name":"HaiYaoDENG","display_name":"Hai-Yao DENG","profile_url":"https://manchester.academia.edu/HaiYaoDENG?f_ri=34232","photo":"https://0.academia-photos.com/100272/27632/25446/s65_hai-yao.deng.jpg"}</script></span></span></li><li class="js-paper-rank-work_1174603 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="1174603"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 1174603, container: ".js-paper-rank-work_1174603", }); });</script></li><li class="js-percentile-work_1174603 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 1174603; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_1174603"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_1174603 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="1174603"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 1174603; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=1174603]").text(description); $(".js-view-count-work_1174603").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_1174603").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="1174603"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">5</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a>, <script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="51549" rel="nofollow" href="https://www.academia.edu/Documents/in/Ferroelectrics">Ferroelectrics</a>, <script data-card-contents-for-ri="51549" type="text/json">{"id":51549,"name":"Ferroelectrics","url":"https://www.academia.edu/Documents/in/Ferroelectrics?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="58003" rel="nofollow" href="https://www.academia.edu/Documents/in/Perovskites">Perovskites</a>, <script data-card-contents-for-ri="58003" type="text/json">{"id":58003,"name":"Perovskites","url":"https://www.academia.edu/Documents/in/Perovskites?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="70946" rel="nofollow" href="https://www.academia.edu/Documents/in/AC_losses_in_superconductors">AC losses in superconductors</a><script data-card-contents-for-ri="70946" type="text/json">{"id":70946,"name":"AC losses in superconductors","url":"https://www.academia.edu/Documents/in/AC_losses_in_superconductors?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=1174603]'), work: {"id":1174603,"title":"Modeling the dielectric behaviors of perovskites : ferroelectrics and incipient ferroelectrics","created_at":"2011-12-22T12:50:13.876-08:00","url":"https://www.academia.edu/1174603/Modeling_the_dielectric_behaviors_of_perovskites_ferroelectrics_and_incipient_ferroelectrics?f_ri=34232","dom_id":"work_1174603","summary":null,"downloadable_attachments":[{"id":21734197,"asset_id":1174603,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":100272,"first_name":"Hai-Yao","last_name":"DENG","domain_name":"manchester","page_name":"HaiYaoDENG","display_name":"Hai-Yao DENG","profile_url":"https://manchester.academia.edu/HaiYaoDENG?f_ri=34232","photo":"https://0.academia-photos.com/100272/27632/25446/s65_hai-yao.deng.jpg"}],"research_interests":[{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":51549,"name":"Ferroelectrics","url":"https://www.academia.edu/Documents/in/Ferroelectrics?f_ri=34232","nofollow":true},{"id":58003,"name":"Perovskites","url":"https://www.academia.edu/Documents/in/Perovskites?f_ri=34232","nofollow":true},{"id":70946,"name":"AC losses in superconductors","url":"https://www.academia.edu/Documents/in/AC_losses_in_superconductors?f_ri=34232","nofollow":true},{"id":342501,"name":"Incipient Ferroelectrics","url":"https://www.academia.edu/Documents/in/Incipient_Ferroelectrics?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_36694855" data-work_id="36694855" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/36694855/High_Tc_Superconductivity_in_Cu_Oxides">High-Tc Superconductivity in Cu Oxides</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Several findings in the area of copper oxide high-Tc superconductivity are shown; from the first high-Tc cuprate superconductor at 30 k, to a Barium-Itrium-doped cuprate superconducting at around 90 K. The main structure of said compound... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_36694855" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Several findings in the area of copper oxide high-Tc superconductivity are shown; from the first high-Tc cuprate superconductor at 30 k, to a Barium-Itrium-doped cuprate superconducting at around 90 K. The main structure of said compound and the systematic analysis for each one are explained and the preparation methods for some of them are exposed. Finally, the theories attempting to describe the superconducting behavior at said temperatures are examined and briefly explained.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/36694855" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="7ab7b648d9632a372a2b1f786e4997aa" rel="nofollow" data-download="{"attachment_id":56633776,"asset_id":36694855,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/56633776/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="64479471" href="https://yachaytech.academia.edu/DavidEliseoLajonesZapata">David Eliseo Lajones Zapata</a><script data-card-contents-for-user="64479471" type="text/json">{"id":64479471,"first_name":"David Eliseo","last_name":"Lajones Zapata","domain_name":"yachaytech","page_name":"DavidEliseoLajonesZapata","display_name":"David Eliseo Lajones Zapata","profile_url":"https://yachaytech.academia.edu/DavidEliseoLajonesZapata?f_ri=34232","photo":"https://0.academia-photos.com/64479471/16759173/17026211/s65_david_eliseo.lajones_zapata.jpg"}</script></span></span></li><li class="js-paper-rank-work_36694855 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="36694855"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 36694855, container: ".js-paper-rank-work_36694855", }); 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$(".js-view-count[data-work-id=36694855]").text(description); $(".js-view-count-work_36694855").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_36694855").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="36694855"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">3</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="6469" rel="nofollow" href="https://www.academia.edu/Documents/in/Superconductivity">Superconductivity</a>, <script data-card-contents-for-ri="6469" type="text/json">{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a>, <script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="99109" rel="nofollow" href="https://www.academia.edu/Documents/in/Cuprate_Superconductors">Cuprate Superconductors</a><script data-card-contents-for-ri="99109" type="text/json">{"id":99109,"name":"Cuprate Superconductors","url":"https://www.academia.edu/Documents/in/Cuprate_Superconductors?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=36694855]'), work: {"id":36694855,"title":"High-Tc Superconductivity in Cu Oxides","created_at":"2018-05-22T18:11:59.445-07:00","url":"https://www.academia.edu/36694855/High_Tc_Superconductivity_in_Cu_Oxides?f_ri=34232","dom_id":"work_36694855","summary":"Several findings in the area of copper oxide high-Tc superconductivity are shown; from the first high-Tc cuprate superconductor at 30 k, to a Barium-Itrium-doped cuprate superconducting at around 90 K. The main structure of said compound and the systematic analysis for each one are explained and the preparation methods for some of them are exposed. Finally, the theories attempting to describe the superconducting behavior at said temperatures are examined and briefly explained.","downloadable_attachments":[{"id":56633776,"asset_id":36694855,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":64479471,"first_name":"David Eliseo","last_name":"Lajones Zapata","domain_name":"yachaytech","page_name":"DavidEliseoLajonesZapata","display_name":"David Eliseo Lajones Zapata","profile_url":"https://yachaytech.academia.edu/DavidEliseoLajonesZapata?f_ri=34232","photo":"https://0.academia-photos.com/64479471/16759173/17026211/s65_david_eliseo.lajones_zapata.jpg"}],"research_interests":[{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":99109,"name":"Cuprate Superconductors","url":"https://www.academia.edu/Documents/in/Cuprate_Superconductors?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_13750885" data-work_id="13750885" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/13750885/Stationary_Josephson_current_as_a_tool_to_detect_charge_density_waves_in_high_Tc_oxides">Stationary Josephson current as a tool to detect charge density waves in high-Tc oxides</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Nonmonotonic and even sign-changing dependences on the temperature and the doping level were predicted for the stationary Josephson tunnel current Ic between superconductors with d-wave order parameter symmetry and partial gapping by... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_13750885" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Nonmonotonic and even sign-changing dependences on the temperature and the doping level were predicted for the stationary Josephson tunnel current Ic between superconductors with d-wave order parameter symmetry and partial gapping by charge density waves (CDWs). The junction electrodes were considered in the framework of the two-dimensional electron spectrum appropriate to high-Tc cuprates. The non-trivial behavior can be observed for certain relative electrode orientations. Hence, Ic-measurements in wide ranges of doping and temperature may serve as an indicator of CDW existence.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/13750885" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="854cfbd74244553eb040054ec5aa8c73" rel="nofollow" data-download="{"attachment_id":38405017,"asset_id":13750885,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/38405017/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="3159343" href="https://iop-kiev.academia.edu/AlexanderGabovich">Alexander M Gabovich</a><script data-card-contents-for-user="3159343" type="text/json">{"id":3159343,"first_name":"Alexander","last_name":"Gabovich","domain_name":"iop-kiev","page_name":"AlexanderGabovich","display_name":"Alexander M Gabovich","profile_url":"https://iop-kiev.academia.edu/AlexanderGabovich?f_ri=34232","photo":"https://0.academia-photos.com/3159343/1074807/1341057/s65_alexander.gabovich.jpg"}</script></span></span></li><li class="js-paper-rank-work_13750885 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="13750885"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 13750885, container: ".js-paper-rank-work_13750885", }); 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$(".js-view-count[data-work-id=13750885]").text(description); $(".js-view-count-work_13750885").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_13750885").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="13750885"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i></div><span class="InlineList-item-text u-textTruncate u-pl6x"><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (false) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=13750885]'), work: {"id":13750885,"title":"Stationary Josephson current as a tool to detect charge density waves in high-Tc oxides","created_at":"2015-07-07T08:02:50.634-07:00","url":"https://www.academia.edu/13750885/Stationary_Josephson_current_as_a_tool_to_detect_charge_density_waves_in_high_Tc_oxides?f_ri=34232","dom_id":"work_13750885","summary":"Nonmonotonic and even sign-changing dependences on the temperature and the doping level were predicted for the stationary Josephson tunnel current Ic between superconductors with d-wave order parameter symmetry and partial gapping by charge density waves (CDWs). The junction electrodes were considered in the framework of the two-dimensional electron spectrum appropriate to high-Tc cuprates. The non-trivial behavior can be observed for certain relative electrode orientations. Hence, Ic-measurements in wide ranges of doping and temperature may serve as an indicator of CDW existence.","downloadable_attachments":[{"id":38405017,"asset_id":13750885,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":3159343,"first_name":"Alexander","last_name":"Gabovich","domain_name":"iop-kiev","page_name":"AlexanderGabovich","display_name":"Alexander M Gabovich","profile_url":"https://iop-kiev.academia.edu/AlexanderGabovich?f_ri=34232","photo":"https://0.academia-photos.com/3159343/1074807/1341057/s65_alexander.gabovich.jpg"}],"research_interests":[{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_1192080" data-work_id="1192080" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/1192080/Pairing_in_disordered_s_wave_superconductors_and_the_effect_of_their_coupling">Pairing in disordered s-wave superconductors and the effect of their coupling</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Inhomogeneity is introduced through random local interactions (U i ) in an attractive Hubbard model on a square lattice and studied using mean-field Bogoliubov-de Gennes formalism. Superconductivity is found to get suppressed by the... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_1192080" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Inhomogeneity is introduced through random local interactions (U i ) in an attractive Hubbard model on a square lattice and studied using mean-field Bogoliubov-de Gennes formalism. Superconductivity is found to get suppressed by the random U i contrary to the results of a bimodal distribution of U i . The proximity effect of superconductivity is found to be strong, all sites develop non-zero pairing amplitude. The gap in the density of states is always non-zero and does not vanish even for strong disorder. When two such superconductors are coupled via a channel, the effect of one on the other is negligible. The length and width of the connector, do not seem to have any noticeable effect on the superconductivity in either systems. The superconducting blocks behave as independent entity and the introduction of the channel have no effect on them.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/1192080" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="16b6081fb5b461d8ed0dd87c3b391ff5" rel="nofollow" data-download="{"attachment_id":7382582,"asset_id":1192080,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/7382582/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="1085913" href="https://uni-hamburg.academia.edu/BudhadityaChatterjee">Budhaditya Chatterjee</a><script data-card-contents-for-user="1085913" type="text/json">{"id":1085913,"first_name":"Budhaditya","last_name":"Chatterjee","domain_name":"uni-hamburg","page_name":"BudhadityaChatterjee","display_name":"Budhaditya Chatterjee","profile_url":"https://uni-hamburg.academia.edu/BudhadityaChatterjee?f_ri=34232","photo":"https://0.academia-photos.com/1085913/376558/456259/s65_budhaditya.chatterjee.jpg"}</script></span></span></li><li class="js-paper-rank-work_1192080 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="1192080"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 1192080, container: ".js-paper-rank-work_1192080", }); 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$(".js-view-count[data-work-id=1192080]").text(description); $(".js-view-count-work_1192080").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_1192080").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="1192080"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">3</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="6469" rel="nofollow" href="https://www.academia.edu/Documents/in/Superconductivity">Superconductivity</a>, <script data-card-contents-for-ri="6469" type="text/json">{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="16400" rel="nofollow" href="https://www.academia.edu/Documents/in/Disordered_Systems">Disordered Systems</a>, <script data-card-contents-for-ri="16400" type="text/json">{"id":16400,"name":"Disordered Systems","url":"https://www.academia.edu/Documents/in/Disordered_Systems?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=1192080]'), work: {"id":1192080,"title":"Pairing in disordered s-wave superconductors and the effect of their coupling","created_at":"2012-01-01T16:42:05.114-08:00","url":"https://www.academia.edu/1192080/Pairing_in_disordered_s_wave_superconductors_and_the_effect_of_their_coupling?f_ri=34232","dom_id":"work_1192080","summary":"Inhomogeneity is introduced through random local interactions (U i ) in an attractive Hubbard model on a square lattice and studied using mean-field Bogoliubov-de Gennes formalism. Superconductivity is found to get suppressed by the random U i contrary to the results of a bimodal distribution of U i . The proximity effect of superconductivity is found to be strong, all sites develop non-zero pairing amplitude. The gap in the density of states is always non-zero and does not vanish even for strong disorder. When two such superconductors are coupled via a channel, the effect of one on the other is negligible. The length and width of the connector, do not seem to have any noticeable effect on the superconductivity in either systems. The superconducting blocks behave as independent entity and the introduction of the channel have no effect on them.","downloadable_attachments":[{"id":7382582,"asset_id":1192080,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":1085913,"first_name":"Budhaditya","last_name":"Chatterjee","domain_name":"uni-hamburg","page_name":"BudhadityaChatterjee","display_name":"Budhaditya Chatterjee","profile_url":"https://uni-hamburg.academia.edu/BudhadityaChatterjee?f_ri=34232","photo":"https://0.academia-photos.com/1085913/376558/456259/s65_budhaditya.chatterjee.jpg"}],"research_interests":[{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true},{"id":16400,"name":"Disordered Systems","url":"https://www.academia.edu/Documents/in/Disordered_Systems?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_38435581 coauthored" data-work_id="38435581" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/38435581/Doping_dependence_of_fluctuation_diamagnetism_in_high_Tc_superconductors">Doping dependence of fluctuation diamagnetism in high Tc superconductors</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Using a recently proposed Ginzburg–Landau-like lattice free energy functional due to Banerjee et al. (2011) we calculate the fluctuation diamagnetism of high-T c superconductors as a function of doping, magnetic field and temperature. We... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_38435581" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Using a recently proposed Ginzburg–Landau-like lattice free energy functional due to Banerjee et al. (2011) we calculate the fluctuation diamagnetism of high-T c superconductors as a function of<br />doping, magnetic field and temperature. We analyse the pairing<br />fluctuations above the superconducting transition temperature in<br />the cuprates, ranging from the strong phase fluctuation dominated<br />underdoped limit to the more conventional amplitude fluctuation<br />dominated overdoped regime. We show that a model where the<br />pairing scale increases and the superfluid density decreases with<br />underdoping produces features of the observed magnetization in<br />the pseudogap region, in good qualitative and reasonable quantitative agreement with the experimental data. In particular, we explicitly show that even when the pseudogap has a pairing origin the<br />magnetization actually tracks the superconducting dome instead of<br />the pseudogap temperature, as seen in experiment. We discuss the<br />doping dependence of the ‘onset’ temperature for fluctuation dia-<br />magnetism and comment on the role of vortex core-energy in our<br />model.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/38435581" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="79ffacd07a08ffd5fbd59f30da1b7dc2" rel="nofollow" data-download="{"attachment_id":58496635,"asset_id":38435581,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/58496635/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="98699526" href="https://vit.academia.edu/KingshukSarkar">Kingshuk Sarkar</a><script data-card-contents-for-user="98699526" type="text/json">{"id":98699526,"first_name":"Kingshuk","last_name":"Sarkar","domain_name":"vit","page_name":"KingshukSarkar","display_name":"Kingshuk Sarkar","profile_url":"https://vit.academia.edu/KingshukSarkar?f_ri=34232","photo":"https://0.academia-photos.com/98699526/22996997/22126497/s65_kingshuk.sarkar.jpg"}</script></span></span><span class="u-displayInlineBlock InlineList-item-text"> and <span class="u-textDecorationUnderline u-clickable InlineList-item-text js-work-more-authors-38435581">+1</span><div class="hidden js-additional-users-38435581"><div><span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a href="https://independent.academia.edu/SumilanBanerjee">Sumilan Banerjee</a></span></div></div></span><script>(function(){ var popoverSettings = { el: $('.js-work-more-authors-38435581'), placement: 'bottom', hide_delay: 200, html: true, content: function(){ return $('.js-additional-users-38435581').html(); 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container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_38435581 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="38435581"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 38435581; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=38435581]").text(description); $(".js-view-count-work_38435581").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_38435581").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="38435581"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">3</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a>, <script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="99109" rel="nofollow" href="https://www.academia.edu/Documents/in/Cuprate_Superconductors">Cuprate Superconductors</a>, <script data-card-contents-for-ri="99109" type="text/json">{"id":99109,"name":"Cuprate Superconductors","url":"https://www.academia.edu/Documents/in/Cuprate_Superconductors?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="179371" rel="nofollow" href="https://www.academia.edu/Documents/in/Pseudogap">Pseudogap</a><script data-card-contents-for-ri="179371" type="text/json">{"id":179371,"name":"Pseudogap","url":"https://www.academia.edu/Documents/in/Pseudogap?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=38435581]'), work: {"id":38435581,"title":"Doping dependence of fluctuation diamagnetism in high Tc superconductors","created_at":"2019-02-25T08:54:10.675-08:00","url":"https://www.academia.edu/38435581/Doping_dependence_of_fluctuation_diamagnetism_in_high_Tc_superconductors?f_ri=34232","dom_id":"work_38435581","summary":"Using a recently proposed Ginzburg–Landau-like lattice free energy functional due to Banerjee et al. (2011) we calculate the fluctuation diamagnetism of high-T c superconductors as a function of\ndoping, magnetic field and temperature. We analyse the pairing\nfluctuations above the superconducting transition temperature in\nthe cuprates, ranging from the strong phase fluctuation dominated\nunderdoped limit to the more conventional amplitude fluctuation\ndominated overdoped regime. We show that a model where the\npairing scale increases and the superfluid density decreases with\nunderdoping produces features of the observed magnetization in\nthe pseudogap region, in good qualitative and reasonable quantitative agreement with the experimental data. In particular, we explicitly show that even when the pseudogap has a pairing origin the\nmagnetization actually tracks the superconducting dome instead of\nthe pseudogap temperature, as seen in experiment. We discuss the\ndoping dependence of the ‘onset’ temperature for fluctuation dia-\nmagnetism and comment on the role of vortex core-energy in our\nmodel.","downloadable_attachments":[{"id":58496635,"asset_id":38435581,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":98699526,"first_name":"Kingshuk","last_name":"Sarkar","domain_name":"vit","page_name":"KingshukSarkar","display_name":"Kingshuk Sarkar","profile_url":"https://vit.academia.edu/KingshukSarkar?f_ri=34232","photo":"https://0.academia-photos.com/98699526/22996997/22126497/s65_kingshuk.sarkar.jpg"},{"id":104177212,"first_name":"Sumilan","last_name":"Banerjee","domain_name":"independent","page_name":"SumilanBanerjee","display_name":"Sumilan Banerjee","profile_url":"https://independent.academia.edu/SumilanBanerjee?f_ri=34232","photo":"https://0.academia-photos.com/104177212/142596812/132100711/s65_sumilan.banerjee.png"}],"research_interests":[{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":99109,"name":"Cuprate Superconductors","url":"https://www.academia.edu/Documents/in/Cuprate_Superconductors?f_ri=34232","nofollow":true},{"id":179371,"name":"Pseudogap","url":"https://www.academia.edu/Documents/in/Pseudogap?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_2272837" data-work_id="2272837" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/2272837/A_Fiber_Bragg_Grating_Bimetal_Temperature_Sensor_for_Solar_Panel_Inverters">A Fiber Bragg GratingBimetal Temperature Sensor for Solar Panel Inverters</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">This paper reports the design, characterization and implementation of a Fiber Bragg Grating (FBG)-based temperature sensor for an Insulted-Gate Bipolar Transistor (IGBT) in a solar panel inverter. The FBG is bonded to the higher... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_2272837" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">This paper reports the design, characterization and implementation of a Fiber Bragg Grating (FBG)-based temperature sensor for an Insulted-Gate Bipolar Transistor (IGBT) in a solar panel inverter. The FBG is bonded to the higher Coefficient of Thermal Expansion (CTE) side of a bimetallic strip to increase its sensitivity. Characterization results show a linear relationship between increasing temperature and the wavelength shift. It is found that the sensitivity of the sensor can be categorized into three characterization temperature regions between 26 degrees C and 90 degrees C. The region from 41 degrees C to 90 degrees C shows the highest sensitivity, with a value of 14 pm/degrees C. A new empirical model that considers both temperature and strain effects has been developed for the sensor. Finally, the FBG-bimetal temperature sensor is placed in a solar panel inverter and results confirm that it can be used for real-time monitoring of the IGBT temperature.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/2272837" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="6b71411c7f95ec4dc068f7daf1a6c572" rel="nofollow" data-download="{"attachment_id":31462401,"asset_id":2272837,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/31462401/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="2869323" href="https://malaya.academia.edu/FaisalRafiqMahamdAdikan">Faisal Rafiq Mahamd Adikan</a><script data-card-contents-for-user="2869323" type="text/json">{"id":2869323,"first_name":"Faisal Rafiq","last_name":"Mahamd Adikan","domain_name":"malaya","page_name":"FaisalRafiqMahamdAdikan","display_name":"Faisal Rafiq Mahamd Adikan","profile_url":"https://malaya.academia.edu/FaisalRafiqMahamdAdikan?f_ri=34232","photo":"https://0.academia-photos.com/2869323/946484/2352011/s65_faisal_rafiq.mahamd_adikan.jpg"}</script></span></span></li><li class="js-paper-rank-work_2272837 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="2272837"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 2272837, container: ".js-paper-rank-work_2272837", }); 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$(".js-view-count[data-work-id=2272837]").text(description); $(".js-view-count-work_2272837").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_2272837").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="2272837"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">5</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a>, <script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="63431" rel="nofollow" href="https://www.academia.edu/Documents/in/Solar_Energy">Solar Energy</a>, <script data-card-contents-for-ri="63431" type="text/json">{"id":63431,"name":"Solar Energy","url":"https://www.academia.edu/Documents/in/Solar_Energy?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="140341" rel="nofollow" href="https://www.academia.edu/Documents/in/Nano-photonics_and_nano-optics_photonic_crystals_integrated_plasmonics_metamaterials_and_their_a">Nano-photonics and nano-optics: photonic crystals, integrated plasmonics, metamaterials, and their applications in quantum computing, quantum/classical communication, sensing</a>, <script data-card-contents-for-ri="140341" type="text/json">{"id":140341,"name":"Nano-photonics and nano-optics: photonic crystals, integrated plasmonics, metamaterials, and their applications in quantum computing, quantum/classical communication, sensing","url":"https://www.academia.edu/Documents/in/Nano-photonics_and_nano-optics_photonic_crystals_integrated_plasmonics_metamaterials_and_their_a?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="875964" rel="nofollow" href="https://www.academia.edu/Documents/in/Silica-on-silicon">Silica-on-silicon</a><script data-card-contents-for-ri="875964" type="text/json">{"id":875964,"name":"Silica-on-silicon","url":"https://www.academia.edu/Documents/in/Silica-on-silicon?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=2272837]'), work: {"id":2272837,"title":"A Fiber Bragg GratingBimetal Temperature Sensor for Solar Panel Inverters","created_at":"2012-12-10T12:13:27.297-08:00","url":"https://www.academia.edu/2272837/A_Fiber_Bragg_Grating_Bimetal_Temperature_Sensor_for_Solar_Panel_Inverters?f_ri=34232","dom_id":"work_2272837","summary":"This paper reports the design, characterization and implementation of a Fiber Bragg Grating (FBG)-based temperature sensor for an Insulted-Gate Bipolar Transistor (IGBT) in a solar panel inverter. The FBG is bonded to the higher Coefficient of Thermal Expansion (CTE) side of a bimetallic strip to increase its sensitivity. Characterization results show a linear relationship between increasing temperature and the wavelength shift. It is found that the sensitivity of the sensor can be categorized into three characterization temperature regions between 26 degrees C and 90 degrees C. The region from 41 degrees C to 90 degrees C shows the highest sensitivity, with a value of 14 pm/degrees C. A new empirical model that considers both temperature and strain effects has been developed for the sensor. Finally, the FBG-bimetal temperature sensor is placed in a solar panel inverter and results confirm that it can be used for real-time monitoring of the IGBT temperature.","downloadable_attachments":[{"id":31462401,"asset_id":2272837,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":2869323,"first_name":"Faisal Rafiq","last_name":"Mahamd Adikan","domain_name":"malaya","page_name":"FaisalRafiqMahamdAdikan","display_name":"Faisal Rafiq Mahamd Adikan","profile_url":"https://malaya.academia.edu/FaisalRafiqMahamdAdikan?f_ri=34232","photo":"https://0.academia-photos.com/2869323/946484/2352011/s65_faisal_rafiq.mahamd_adikan.jpg"}],"research_interests":[{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":63431,"name":"Solar Energy","url":"https://www.academia.edu/Documents/in/Solar_Energy?f_ri=34232","nofollow":true},{"id":140341,"name":"Nano-photonics and nano-optics: photonic crystals, integrated plasmonics, metamaterials, and their applications in quantum computing, quantum/classical communication, sensing","url":"https://www.academia.edu/Documents/in/Nano-photonics_and_nano-optics_photonic_crystals_integrated_plasmonics_metamaterials_and_their_a?f_ri=34232","nofollow":true},{"id":875964,"name":"Silica-on-silicon","url":"https://www.academia.edu/Documents/in/Silica-on-silicon?f_ri=34232","nofollow":true},{"id":875965,"name":"Planar Lightwave","url":"https://www.academia.edu/Documents/in/Planar_Lightwave?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_41588061" data-work_id="41588061" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/41588061/MATERIALES_SUPERCONDUCTORES_EN_BASE_A_HIERRO_LOS_MATERIALES_SUPERCONDUCTORES_MAGN%C3%89TICOS">MATERIALES SUPERCONDUCTORES EN BASE A HIERRO: LOS MATERIALES SUPERCONDUCTORES – MAGNÉTICOS</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Nuevos caminos para estudiar la superconductividad se han abierto en años recientes. Hace unos cuatro años se descubrió que la superconductividad admite la presencia de átomos magnéticos como el hierro, en las estructuras de los... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_41588061" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Nuevos caminos para estudiar la superconductividad se han abierto en años recientes. Hace unos cuatro años se descubrió que la superconductividad admite la presencia de átomos magnéticos como el hierro, en las estructuras de los compuestos. Magnetismo y superconductividad ya no son fenómenos antagónicos en ciertos materiales: conocidos como FeAsSC. La investigación tanto teórica como experimental de este hecho, promete brindar nuevos retos a químicos y físicos, pero también a muchos otros que esperan lograr aplicaciones más amplias de los superconductores de alta temperatura crítica.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/41588061" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="f2b438ea88c45e75f0748e2d1bdb3071" rel="nofollow" data-download="{"attachment_id":61745184,"asset_id":41588061,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/61745184/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="13511020" href="https://uson.academia.edu/RPerezEnriquez">Raul Perez-Enriquez</a><script data-card-contents-for-user="13511020" type="text/json">{"id":13511020,"first_name":"Raul","last_name":"Perez-Enriquez","domain_name":"uson","page_name":"RPerezEnriquez","display_name":"Raul Perez-Enriquez","profile_url":"https://uson.academia.edu/RPerezEnriquez?f_ri=34232","photo":"https://0.academia-photos.com/13511020/18738648/18700015/s65_raul.perez-enriquez.jpg"}</script></span></span></li><li class="js-paper-rank-work_41588061 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="41588061"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 41588061, container: ".js-paper-rank-work_41588061", }); });</script></li><li class="js-percentile-work_41588061 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 41588061; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_41588061"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_41588061 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="41588061"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 41588061; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=41588061]").text(description); $(".js-view-count-work_41588061").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_41588061").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="41588061"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">2</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="7715" rel="nofollow" href="https://www.academia.edu/Documents/in/Magnetic_Materials">Magnetic Materials</a>, <script data-card-contents-for-ri="7715" type="text/json">{"id":7715,"name":"Magnetic Materials","url":"https://www.academia.edu/Documents/in/Magnetic_Materials?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=41588061]'), work: {"id":41588061,"title":"MATERIALES SUPERCONDUCTORES EN BASE A HIERRO: LOS MATERIALES SUPERCONDUCTORES – MAGNÉTICOS","created_at":"2020-01-10T17:16:32.349-08:00","url":"https://www.academia.edu/41588061/MATERIALES_SUPERCONDUCTORES_EN_BASE_A_HIERRO_LOS_MATERIALES_SUPERCONDUCTORES_MAGN%C3%89TICOS?f_ri=34232","dom_id":"work_41588061","summary":"Nuevos caminos para estudiar la superconductividad se han abierto en años recientes. Hace unos cuatro años se descubrió que la superconductividad admite la presencia de átomos magnéticos como el hierro, en las estructuras de los compuestos. Magnetismo y superconductividad ya no son fenómenos antagónicos en ciertos materiales: conocidos como FeAsSC. La investigación tanto teórica como experimental de este hecho, promete brindar nuevos retos a químicos y físicos, pero también a muchos otros que esperan lograr aplicaciones más amplias de los superconductores de alta temperatura crítica.","downloadable_attachments":[{"id":61745184,"asset_id":41588061,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":13511020,"first_name":"Raul","last_name":"Perez-Enriquez","domain_name":"uson","page_name":"RPerezEnriquez","display_name":"Raul Perez-Enriquez","profile_url":"https://uson.academia.edu/RPerezEnriquez?f_ri=34232","photo":"https://0.academia-photos.com/13511020/18738648/18700015/s65_raul.perez-enriquez.jpg"}],"research_interests":[{"id":7715,"name":"Magnetic Materials","url":"https://www.academia.edu/Documents/in/Magnetic_Materials?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_14136414" data-work_id="14136414" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/14136414/Enhanced_Magnetic_Properties_in_Cu0_5_Tl0_5_Ba2_Ca2_Cu3_O10_%CE%B4_Superconductor_Doped_with_Carbon_Nanotubes">Enhanced Magnetic Properties in Cu0.5 Tl0.5 Ba2 Ca2 Cu3 O10−δ Superconductor Doped with Carbon Nanotubes</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Fluctuation-induced conductivity (FIC) analysis in the critical fluctuation region (cr), three-dimensional (3D), two-dimensional (2D), and zero-dimensional (0D) regions is reported for undoped and carbon nanotubes (CNT)-doped... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_14136414" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Fluctuation-induced conductivity (FIC) analysis in the critical fluctuation region (cr), three-dimensional (3D), two-dimensional (2D), and zero-dimensional (0D) regions is reported for undoped and carbon nanotubes (CNT)-doped Cu0.5Tl0.5Ba2Ca2Cu3O10−δ (CuTl-1223) superconductors. Samples were synthesized by well-known solid-state reaction method by adding CNT up to 7 wt %. The X-ray diffraction data confirms the single-phase orthorhombic structures following PMMM space group for all the samples. The scanning electron microscope (SEM) images reveal that the carbon nanotubes are present in the spaces between the grains and connect the grains electrically to help the intergranular current flow. From FIC analysis, it was found that the width of critical and 3D regimes are shrunken with the increased CNT doping in the final compound. Also, the coherence length (ξc(0)), the Fermi velocity (V F), and the coupling constant (J) are suppressed with increased CNT doping except for the 0.25 wt % doped sample. The decrease in important superconductivity parameters most likely arises due to low CNT doping which indeed functions as columnar defects that are produced by heavy ion irradiation. In this analysis, we also found that the critical magnetic fields (B c(0), B c1(0)) and critical current density (J c(0)) were found to increase with increased CNT concentration. These observations suggest that addition of CNT (efficient pinning centers) to CuTl-1223 compounds improve the electrical connection between the superconducting grains to result in the improvement of magnetic properties of the final compound.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/14136414" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="ed730506cf3b32cad8607e6f0a6df5a5" rel="nofollow" data-download="{"attachment_id":38212438,"asset_id":14136414,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/38212438/download_file?st=MTczOTgzMjMyNCw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="5623346" href="https://qau.academia.edu/AftabRafique">Aftab Rafique</a><script data-card-contents-for-user="5623346" type="text/json">{"id":5623346,"first_name":"Aftab","last_name":"Rafique","domain_name":"qau","page_name":"AftabRafique","display_name":"Aftab Rafique","profile_url":"https://qau.academia.edu/AftabRafique?f_ri=34232","photo":"https://0.academia-photos.com/5623346/2450998/10953426/s65_aftab.rafique.png"}</script></span></span></li><li class="js-paper-rank-work_14136414 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="14136414"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 14136414, container: ".js-paper-rank-work_14136414", }); });</script></li><li class="js-percentile-work_14136414 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 14136414; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_14136414"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_14136414 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="14136414"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 14136414; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=14136414]").text(description); $(".js-view-count-work_14136414").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_14136414").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="14136414"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">2</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="6469" rel="nofollow" href="https://www.academia.edu/Documents/in/Superconductivity">Superconductivity</a>, <script data-card-contents-for-ri="6469" type="text/json">{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=14136414]'), work: {"id":14136414,"title":"Enhanced Magnetic Properties in Cu0.5 Tl0.5 Ba2 Ca2 Cu3 O10−δ Superconductor Doped with Carbon Nanotubes","created_at":"2015-07-16T19:30:01.001-07:00","url":"https://www.academia.edu/14136414/Enhanced_Magnetic_Properties_in_Cu0_5_Tl0_5_Ba2_Ca2_Cu3_O10_%CE%B4_Superconductor_Doped_with_Carbon_Nanotubes?f_ri=34232","dom_id":"work_14136414","summary":"Fluctuation-induced conductivity (FIC) analysis in the critical fluctuation region (cr), three-dimensional (3D), two-dimensional (2D), and zero-dimensional (0D) regions is reported for undoped and carbon nanotubes (CNT)-doped Cu0.5Tl0.5Ba2Ca2Cu3O10−δ (CuTl-1223) superconductors. Samples were synthesized by well-known solid-state reaction method by adding CNT up to 7 wt %. The X-ray diffraction data confirms the single-phase orthorhombic structures following PMMM space group for all the samples. The scanning electron microscope (SEM) images reveal that the carbon nanotubes are present in the spaces between the grains and connect the grains electrically to help the intergranular current flow. From FIC analysis, it was found that the width of critical and 3D regimes are shrunken with the increased CNT doping in the final compound. Also, the coherence length (ξc(0)), the Fermi velocity (V F), and the coupling constant (J) are suppressed with increased CNT doping except for the 0.25 wt % doped sample. The decrease in important superconductivity parameters most likely arises due to low CNT doping which indeed functions as columnar defects that are produced by heavy ion irradiation. In this analysis, we also found that the critical magnetic fields (B c(0), B c1(0)) and critical current density (J c(0)) were found to increase with increased CNT concentration. These observations suggest that addition of CNT (efficient pinning centers) to CuTl-1223 compounds improve the electrical connection between the superconducting grains to result in the improvement of magnetic properties of the final compound.","downloadable_attachments":[{"id":38212438,"asset_id":14136414,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":5623346,"first_name":"Aftab","last_name":"Rafique","domain_name":"qau","page_name":"AftabRafique","display_name":"Aftab Rafique","profile_url":"https://qau.academia.edu/AftabRafique?f_ri=34232","photo":"https://0.academia-photos.com/5623346/2450998/10953426/s65_aftab.rafique.png"}],"research_interests":[{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_13258926" data-work_id="13258926" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/13258926/Genesis_of_charge_orders_in_high_temperature_superconductors">Genesis of charge orders in high temperature superconductors</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">One of the most puzzling facts about cuprate high temperature superconductors in the lightly doped regime is the coexistence of the uniform superconductivity and/or antiferromagnetism with a variety of low-energy charge-ordered states in... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_13258926" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">One of the most puzzling facts about cuprate high temperature superconductors in the lightly doped regime is the coexistence of the uniform superconductivity and/or antiferromagnetism with a variety of low-energy charge-ordered states in a unidirectional charge density wave or a bidirectional checkerboard structure. Recent experiments have discovered these charge density waves exhibiting dominant d-like symmetry in their intra-unit-cell form factor. Taking into account the strong local Coulomb repulsion present in cuprates, we use effective interactions to obtain a number of nearly degenerate charge-ordered states. All of them have pair density wave intertwined with a charge density wave and sometimes also with a spin density wave together. Most of these states vanish in the underdoped regime except one with a large d-form factor vanishes around 19% doping of holes as observed[1,2]. These states could coexist with a uniform d-wave superconducting order. The checkerboard state is predicted to have a d-form factor.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/13258926" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="0a0d2494c2cff22731bea7e3649084d3" rel="nofollow" data-download="{"attachment_id":50984808,"asset_id":13258926,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/50984808/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="18807285" href="https://korea-kr.academia.edu/WeiLinTu">Wei-Lin Tu</a><script data-card-contents-for-user="18807285" type="text/json">{"id":18807285,"first_name":"Wei-Lin","last_name":"Tu","domain_name":"korea-kr","page_name":"WeiLinTu","display_name":"Wei-Lin Tu","profile_url":"https://korea-kr.academia.edu/WeiLinTu?f_ri=34232","photo":"https://0.academia-photos.com/18807285/20579331/20196441/s65_wei-lin.tu.jpg"}</script></span></span></li><li class="js-paper-rank-work_13258926 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="13258926"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 13258926, container: ".js-paper-rank-work_13258926", }); });</script></li><li class="js-percentile-work_13258926 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 13258926; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_13258926"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_13258926 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="13258926"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 13258926; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=13258926]").text(description); $(".js-view-count-work_13258926").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_13258926").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="13258926"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">3</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="505" rel="nofollow" href="https://www.academia.edu/Documents/in/Condensed_Matter_Physics">Condensed Matter Physics</a>, <script data-card-contents-for-ri="505" type="text/json">{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="32745" rel="nofollow" href="https://www.academia.edu/Documents/in/Strongly-correlated_electron_systems">Strongly-correlated electron systems</a>, <script data-card-contents-for-ri="32745" type="text/json">{"id":32745,"name":"Strongly-correlated electron systems","url":"https://www.academia.edu/Documents/in/Strongly-correlated_electron_systems?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=13258926]'), work: {"id":13258926,"title":"Genesis of charge orders in high temperature superconductors","created_at":"2015-06-24T22:09:03.550-07:00","url":"https://www.academia.edu/13258926/Genesis_of_charge_orders_in_high_temperature_superconductors?f_ri=34232","dom_id":"work_13258926","summary":"One of the most puzzling facts about cuprate high temperature superconductors in the lightly doped regime is the coexistence of the uniform superconductivity and/or antiferromagnetism with a variety of low-energy charge-ordered states in a unidirectional charge density wave or a bidirectional checkerboard structure. Recent experiments have discovered these charge density waves exhibiting dominant d-like symmetry in their intra-unit-cell form factor. Taking into account the strong local Coulomb repulsion present in cuprates, we use effective interactions to obtain a number of nearly degenerate charge-ordered states. All of them have pair density wave intertwined with a charge density wave and sometimes also with a spin density wave together. Most of these states vanish in the underdoped regime except one with a large d-form factor vanishes around 19% doping of holes as observed[1,2]. These states could coexist with a uniform d-wave superconducting order. The checkerboard state is predicted to have a d-form factor.","downloadable_attachments":[{"id":50984808,"asset_id":13258926,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":18807285,"first_name":"Wei-Lin","last_name":"Tu","domain_name":"korea-kr","page_name":"WeiLinTu","display_name":"Wei-Lin Tu","profile_url":"https://korea-kr.academia.edu/WeiLinTu?f_ri=34232","photo":"https://0.academia-photos.com/18807285/20579331/20196441/s65_wei-lin.tu.jpg"}],"research_interests":[{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics?f_ri=34232","nofollow":true},{"id":32745,"name":"Strongly-correlated electron systems","url":"https://www.academia.edu/Documents/in/Strongly-correlated_electron_systems?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_9811530" data-work_id="9811530" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/9811530/Three_dimensional_magnetic_structures_and_rare_earth_magnetic_ordering_in_Nd2CuO4_and_Pr2CuO4">Three-dimensional magnetic structures and rare-earth magnetic ordering in Nd2CuO4 and Pr2CuO4</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">The three-dimensional (3D) magnetism present in Nd2CuO4 and Pr2CuO4 has been examined in neutron-scattering experiments. Antiferromagnetic long-range order of the Cu2+ moments develops below TN=255 K in both compounds. In Nd2CuO4 a series... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_9811530" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">The three-dimensional (3D) magnetism present in Nd2CuO4 and Pr2CuO4 has been examined in neutron-scattering experiments. Antiferromagnetic long-range order of the Cu2+ moments develops below TN=255 K in both compounds. In Nd2CuO4 a series of magnetic phase transitions in which the Cu2+ spins reorient has also been observed below TN, while in Pr2CuO4 the 3D Cu2+ spin structure is stable. No changes in the crystalline structure of Nd2CuO4 associated with the spin-reorientation transitions were found. Induced ordering of the rare-earth magnetic moments has been observed in both compounds. The Nd3+ (Pr3+) magnetic moments align parallel (antiparallel) to Cu2+ moments which are nearest neighbors along the c axis, and the ordered moments of the rare-earth ions were determined to be ∼1.3 μB for Nd3+ at 0.4 K and ∼0.08 μB for Pr3+ at 8 K. The temperature-dependent Pr3+ moment is shown to be proportional to the Cu2+ moment times the bulk susceptibility. In this paper we also discuss the role of the XY anisotropy in the 3D ordering.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/9811530" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="650c25d5c431d8477eb6f17268258d1f" rel="nofollow" data-download="{"attachment_id":35982240,"asset_id":9811530,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/35982240/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="13892283" href="https://nist.academia.edu/PeterGehring">Peter Gehring</a><script data-card-contents-for-user="13892283" type="text/json">{"id":13892283,"first_name":"Peter","last_name":"Gehring","domain_name":"nist","page_name":"PeterGehring","display_name":"Peter Gehring","profile_url":"https://nist.academia.edu/PeterGehring?f_ri=34232","photo":"https://0.academia-photos.com/13892283/3853712/4508620/s65_peter.gehring.jpg"}</script></span></span></li><li class="js-paper-rank-work_9811530 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="9811530"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 9811530, container: ".js-paper-rank-work_9811530", }); });</script></li><li class="js-percentile-work_9811530 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 9811530; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_9811530"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_9811530 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="9811530"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 9811530; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=9811530]").text(description); $(".js-view-count-work_9811530").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_9811530").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="9811530"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i></div><span class="InlineList-item-text u-textTruncate u-pl6x"><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a><script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (false) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=9811530]'), work: {"id":9811530,"title":"Three-dimensional magnetic structures and rare-earth magnetic ordering in Nd2CuO4 and Pr2CuO4","created_at":"2014-12-17T06:49:37.912-08:00","url":"https://www.academia.edu/9811530/Three_dimensional_magnetic_structures_and_rare_earth_magnetic_ordering_in_Nd2CuO4_and_Pr2CuO4?f_ri=34232","dom_id":"work_9811530","summary":"The three-dimensional (3D) magnetism present in Nd2CuO4 and Pr2CuO4 has been examined in neutron-scattering experiments. Antiferromagnetic long-range order of the Cu2+ moments develops below TN=255 K in both compounds. In Nd2CuO4 a series of magnetic phase transitions in which the Cu2+ spins reorient has also been observed below TN, while in Pr2CuO4 the 3D Cu2+ spin structure is stable. No changes in the crystalline structure of Nd2CuO4 associated with the spin-reorientation transitions were found. Induced ordering of the rare-earth magnetic moments has been observed in both compounds. The Nd3+ (Pr3+) magnetic moments align parallel (antiparallel) to Cu2+ moments which are nearest neighbors along the c axis, and the ordered moments of the rare-earth ions were determined to be ∼1.3 μB for Nd3+ at 0.4 K and ∼0.08 μB for Pr3+ at 8 K. The temperature-dependent Pr3+ moment is shown to be proportional to the Cu2+ moment times the bulk susceptibility. In this paper we also discuss the role of the XY anisotropy in the 3D ordering.","downloadable_attachments":[{"id":35982240,"asset_id":9811530,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":13892283,"first_name":"Peter","last_name":"Gehring","domain_name":"nist","page_name":"PeterGehring","display_name":"Peter Gehring","profile_url":"https://nist.academia.edu/PeterGehring?f_ri=34232","photo":"https://0.academia-photos.com/13892283/3853712/4508620/s65_peter.gehring.jpg"}],"research_interests":[{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_175186" data-work_id="175186" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/175186/A_Monte_Carlo_study_of_proximity_effects_in_electron_beam_Patterning_of_HTS_Thin_Films">A Monte Carlo study of proximity effects in electron-beam Patterning of HTS Thin Films</a></div></div><div class="u-pb4x u-mt3x"></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/175186" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="7ee4fca8a79f2846542da9d04b12e47f" rel="nofollow" data-download="{"attachment_id":107592,"asset_id":175186,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/107592/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="35107" href="https://hzdr.academia.edu/YordanGeorgiev">Yordan M Georgiev</a><script data-card-contents-for-user="35107" 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{ var workId = 175186; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_175186"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_175186 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="175186"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 175186; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=175186]").text(description); $(".js-view-count-work_175186").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_175186").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="175186"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">7</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="3988" rel="nofollow" href="https://www.academia.edu/Documents/in/Nanoelectronics">Nanoelectronics</a>, <script data-card-contents-for-ri="3988" type="text/json">{"id":3988,"name":"Nanoelectronics","url":"https://www.academia.edu/Documents/in/Nanoelectronics?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="4392" rel="nofollow" href="https://www.academia.edu/Documents/in/Monte_Carlo_Simulation">Monte Carlo Simulation</a>, <script data-card-contents-for-ri="4392" 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$('*[data-has-card-for-ri-list=175186]'), work: {"id":175186,"title":"A Monte Carlo study of proximity effects in electron-beam Patterning of HTS Thin Films","created_at":"2009-03-13T22:39:05.351-07:00","url":"https://www.academia.edu/175186/A_Monte_Carlo_study_of_proximity_effects_in_electron_beam_Patterning_of_HTS_Thin_Films?f_ri=34232","dom_id":"work_175186","summary":null,"downloadable_attachments":[{"id":107592,"asset_id":175186,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":35107,"first_name":"Yordan","last_name":"Georgiev","domain_name":"hzdr","page_name":"YordanGeorgiev","display_name":"Yordan M Georgiev","profile_url":"https://hzdr.academia.edu/YordanGeorgiev?f_ri=34232","photo":"https://0.academia-photos.com/35107/11551/10867/s65_yordan.georgiev.jpg"}],"research_interests":[{"id":3988,"name":"Nanoelectronics","url":"https://www.academia.edu/Documents/in/Nanoelectronics?f_ri=34232","nofollow":true},{"id":4392,"name":"Monte Carlo 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itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/24666010/Magnetic_and_structural_instabilities_in_the_stripe_phase_region_of_La_1_875_Ba_0_125_y_Sr_y_CuO_4_0_y_0_1">Magnetic and structural instabilities in the stripe-phase region of La 1.875 Ba 0.125−y Sr y CuO 4 (0 y 0.1</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Zero-field positive muon spin relaxation (ZF-µ + SR) experiments were performed to investigate the magnetic properties of the low-temperature structural modifications of the La 1.875 Ba 0.125−y Sr y CuO 4 (y = 0.0, 0.025, 0.050, 0.075,... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_24666010" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Zero-field positive muon spin relaxation (ZF-µ + SR) experiments were performed to investigate the magnetic properties of the low-temperature structural modifications of the La 1.875 Ba 0.125−y Sr y CuO 4 (y = 0.0, 0.025, 0.050, 0.075, 0.100) series, in which the total hole concentration is close to 1/8. Together with high-resolution time-of-flight neutron powder diffraction measurements, the results imply that the interplay among lattice distortions, doping and superconductivity is intimately related to the magnetic correlations of the Cu spins, which are interpreted in terms of a stripe-phase model. Materials with y 0.075 exhibit an incomplete structural transition at T d2 , from a low-temperature orthorhombic (LTO, Bmab) to a low-temperature tetragonal (LTT, P 4 2 /ncm) phase. Diffraction patterns collected while approaching T d2 reveal a rapid reduction of the orthorhombicity in the LTO phase with a residual fraction always surviving to low temperatures. Different behaviour is shown by the composition with y = 0.1. Rietveld analysis shows coexistence of the LTO phase with a less distorted low-temperature orthorhombic phase (LTO-2, P ccn). In the LTT phase, a fraction of muons senses regions with purely static spin correlations due to an incommensurate spin-density wave. The muon spin depolarization suggests that in the spatially separated remnant LTO, hole-rich domains, dynamical correlations of charge density give rise to superconductivity. As the spin fluctuations become static at y 0.075, the London penetration depth, λ calculated from the transverse-field µ + SR depolarization rate, σ (T → 0) ∝ λ −2 ∝ n s /m * , reveals a decrease in the superconducting carrier density. The magnetic freezing temperature, T f is suppressed and the magnetic phase fraction shrinks as y increases, whereas the superconducting correlations persist in a larger sample volume. The disappearance of long-range magnetic order at y = 0.1 and the growth of a quasi-static component correlate well with the presence of the LTO-2 microstructure which behaves as a buffer phase out of which the LTT domains become dominant in the Ba-rich compositions.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/24666010" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="46cab16e494fea44f17bac25e777c42f" rel="nofollow" data-download="{"attachment_id":44993551,"asset_id":24666010,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/44993551/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="35689679" href="https://forth.academia.edu/AlexandrosLappas">Alexandros Lappas</a><script data-card-contents-for-user="35689679" type="text/json">{"id":35689679,"first_name":"Alexandros","last_name":"Lappas","domain_name":"forth","page_name":"AlexandrosLappas","display_name":"Alexandros Lappas","profile_url":"https://forth.academia.edu/AlexandrosLappas?f_ri=34232","photo":"https://0.academia-photos.com/35689679/10516599/11735291/s65_alexandros.lappas.jpg"}</script></span></span></li><li class="js-paper-rank-work_24666010 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="24666010"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 24666010, container: ".js-paper-rank-work_24666010", }); 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$(".js-view-count[data-work-id=24666010]").text(description); $(".js-view-count-work_24666010").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_24666010").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="24666010"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">4</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="7715" rel="nofollow" href="https://www.academia.edu/Documents/in/Magnetic_Materials">Magnetic Materials</a>, <script data-card-contents-for-ri="7715" type="text/json">{"id":7715,"name":"Magnetic Materials","url":"https://www.academia.edu/Documents/in/Magnetic_Materials?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="21553" rel="nofollow" href="https://www.academia.edu/Documents/in/Neutron_Diffraction">Neutron Diffraction</a>, <script data-card-contents-for-ri="21553" type="text/json">{"id":21553,"name":"Neutron Diffraction","url":"https://www.academia.edu/Documents/in/Neutron_Diffraction?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a>, <script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="240738" rel="nofollow" href="https://www.academia.edu/Documents/in/Muon_Spin_Relaxation_Resonance_and_Rotation">Muon Spin Relaxation, Resonance and Rotation</a><script data-card-contents-for-ri="240738" type="text/json">{"id":240738,"name":"Muon Spin Relaxation, Resonance and Rotation","url":"https://www.academia.edu/Documents/in/Muon_Spin_Relaxation_Resonance_and_Rotation?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=24666010]'), work: {"id":24666010,"title":"Magnetic and structural instabilities in the stripe-phase region of La 1.875 Ba 0.125−y Sr y CuO 4 (0 y 0.1","created_at":"2016-04-22T11:25:28.884-07:00","url":"https://www.academia.edu/24666010/Magnetic_and_structural_instabilities_in_the_stripe_phase_region_of_La_1_875_Ba_0_125_y_Sr_y_CuO_4_0_y_0_1?f_ri=34232","dom_id":"work_24666010","summary":"Zero-field positive muon spin relaxation (ZF-µ + SR) experiments were performed to investigate the magnetic properties of the low-temperature structural modifications of the La 1.875 Ba 0.125−y Sr y CuO 4 (y = 0.0, 0.025, 0.050, 0.075, 0.100) series, in which the total hole concentration is close to 1/8. Together with high-resolution time-of-flight neutron powder diffraction measurements, the results imply that the interplay among lattice distortions, doping and superconductivity is intimately related to the magnetic correlations of the Cu spins, which are interpreted in terms of a stripe-phase model. Materials with y 0.075 exhibit an incomplete structural transition at T d2 , from a low-temperature orthorhombic (LTO, Bmab) to a low-temperature tetragonal (LTT, P 4 2 /ncm) phase. Diffraction patterns collected while approaching T d2 reveal a rapid reduction of the orthorhombicity in the LTO phase with a residual fraction always surviving to low temperatures. Different behaviour is shown by the composition with y = 0.1. Rietveld analysis shows coexistence of the LTO phase with a less distorted low-temperature orthorhombic phase (LTO-2, P ccn). In the LTT phase, a fraction of muons senses regions with purely static spin correlations due to an incommensurate spin-density wave. The muon spin depolarization suggests that in the spatially separated remnant LTO, hole-rich domains, dynamical correlations of charge density give rise to superconductivity. As the spin fluctuations become static at y 0.075, the London penetration depth, λ calculated from the transverse-field µ + SR depolarization rate, σ (T → 0) ∝ λ −2 ∝ n s /m * , reveals a decrease in the superconducting carrier density. The magnetic freezing temperature, T f is suppressed and the magnetic phase fraction shrinks as y increases, whereas the superconducting correlations persist in a larger sample volume. The disappearance of long-range magnetic order at y = 0.1 and the growth of a quasi-static component correlate well with the presence of the LTO-2 microstructure which behaves as a buffer phase out of which the LTT domains become dominant in the Ba-rich compositions.","downloadable_attachments":[{"id":44993551,"asset_id":24666010,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":35689679,"first_name":"Alexandros","last_name":"Lappas","domain_name":"forth","page_name":"AlexandrosLappas","display_name":"Alexandros Lappas","profile_url":"https://forth.academia.edu/AlexandrosLappas?f_ri=34232","photo":"https://0.academia-photos.com/35689679/10516599/11735291/s65_alexandros.lappas.jpg"}],"research_interests":[{"id":7715,"name":"Magnetic Materials","url":"https://www.academia.edu/Documents/in/Magnetic_Materials?f_ri=34232","nofollow":true},{"id":21553,"name":"Neutron Diffraction","url":"https://www.academia.edu/Documents/in/Neutron_Diffraction?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":240738,"name":"Muon Spin Relaxation, Resonance and Rotation","url":"https://www.academia.edu/Documents/in/Muon_Spin_Relaxation_Resonance_and_Rotation?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_22652408" data-work_id="22652408" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/22652408/The_origins_of_macroscopic_quantum_coherence_in_high_temperature_superconductivity">The origins of macroscopic quantum coherence in high temperature superconductivity</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">A new, theoretical approach to macroscopic quantum coherence and superconduc-tivity in the p-type (hole doped) cuprates is proposed. The theory includes mechanisms to account for e-pair coupling in the superconducting and pseudogap phases... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_22652408" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">A new, theoretical approach to macroscopic quantum coherence and superconduc-tivity in the p-type (hole doped) cuprates is proposed. The theory includes mechanisms to account for e-pair coupling in the superconducting and pseudogap phases and their inter relations observed in these materials. Electron pair coupling in the superconducting phase is facilitated by local quantum potentials created by static dopants in a mechanism which explains experimentally observed optimal doping levels and the associated peak in critical temperature. By contrast, evidence suggests that electrons contributing to the pseudogap are predominantly coupled by fractal spin waves (fractons) induced by the fractal arrangement of dopants. On another level, the theory offers new insights into the emergence of a macro-scopic quantum potential generated by a fractal distribution of dopants. This, in turn, leads to the emergence of coherent, macroscopic spin waves and a second associated macroscopic quantum potential, possibly supported by charge order. These quantum potentials play two key roles. The first involves the transition of an expected diffu-sive process (normally associated with Anderson localization) in fractal networks, into e-pair coherence. The second involves the facilitation of tunnelling between localized e-pairs. These combined effects lead to the merger of the super conducting and pseudo gap phases into a single coherent condensate at optimal doping. The underlying theory relating to the diffusion to quantum transition is supported by Coherent Random Lasing, which can be explained using an analogous approach. As a final step, an experimental program is outlined to validate the theory and suggests a new approach to increase the stability of electron pair condensates at higher temperatures.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/22652408" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="2ccd7e3e991dc7c5415fb4650ee38f17" rel="nofollow" data-download="{"attachment_id":43243500,"asset_id":22652408,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/43243500/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="25454076" href="https://independent.academia.edu/Philipturner8">Philip turner</a><script data-card-contents-for-user="25454076" type="text/json">{"id":25454076,"first_name":"Philip","last_name":"turner","domain_name":"independent","page_name":"Philipturner8","display_name":"Philip turner","profile_url":"https://independent.academia.edu/Philipturner8?f_ri=34232","photo":"https://0.academia-photos.com/25454076/11783821/13135073/s65_philip.turner.jpg"}</script></span></span></li><li class="js-paper-rank-work_22652408 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="22652408"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 22652408, container: ".js-paper-rank-work_22652408", }); 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$(".js-view-count[data-work-id=22652408]").text(description); $(".js-view-count-work_22652408").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_22652408").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="22652408"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">10</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="317" rel="nofollow" href="https://www.academia.edu/Documents/in/Fractal_Geometry">Fractal Geometry</a>, <script data-card-contents-for-ri="317" type="text/json">{"id":317,"name":"Fractal Geometry","url":"https://www.academia.edu/Documents/in/Fractal_Geometry?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="3396" rel="nofollow" href="https://www.academia.edu/Documents/in/Foundations_of_Quantum_Mechanics">Foundations of Quantum Mechanics</a>, <script data-card-contents-for-ri="3396" type="text/json">{"id":3396,"name":"Foundations of Quantum Mechanics","url":"https://www.academia.edu/Documents/in/Foundations_of_Quantum_Mechanics?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="3504" rel="nofollow" href="https://www.academia.edu/Documents/in/General_Relativity">General Relativity</a>, <script data-card-contents-for-ri="3504" type="text/json">{"id":3504,"name":"General Relativity","url":"https://www.academia.edu/Documents/in/General_Relativity?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="7936" rel="nofollow" href="https://www.academia.edu/Documents/in/Quantum_Mechanics">Quantum Mechanics</a><script data-card-contents-for-ri="7936" type="text/json">{"id":7936,"name":"Quantum Mechanics","url":"https://www.academia.edu/Documents/in/Quantum_Mechanics?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=22652408]'), work: {"id":22652408,"title":"The origins of macroscopic quantum coherence in high temperature superconductivity","created_at":"2016-03-01T07:37:46.144-08:00","url":"https://www.academia.edu/22652408/The_origins_of_macroscopic_quantum_coherence_in_high_temperature_superconductivity?f_ri=34232","dom_id":"work_22652408","summary":"A new, theoretical approach to macroscopic quantum coherence and superconduc-tivity in the p-type (hole doped) cuprates is proposed. The theory includes mechanisms to account for e-pair coupling in the superconducting and pseudogap phases and their inter relations observed in these materials. Electron pair coupling in the superconducting phase is facilitated by local quantum potentials created by static dopants in a mechanism which explains experimentally observed optimal doping levels and the associated peak in critical temperature. By contrast, evidence suggests that electrons contributing to the pseudogap are predominantly coupled by fractal spin waves (fractons) induced by the fractal arrangement of dopants. On another level, the theory offers new insights into the emergence of a macro-scopic quantum potential generated by a fractal distribution of dopants. This, in turn, leads to the emergence of coherent, macroscopic spin waves and a second associated macroscopic quantum potential, possibly supported by charge order. These quantum potentials play two key roles. The first involves the transition of an expected diffu-sive process (normally associated with Anderson localization) in fractal networks, into e-pair coherence. The second involves the facilitation of tunnelling between localized e-pairs. These combined effects lead to the merger of the super conducting and pseudo gap phases into a single coherent condensate at optimal doping. The underlying theory relating to the diffusion to quantum transition is supported by Coherent Random Lasing, which can be explained using an analogous approach. As a final step, an experimental program is outlined to validate the theory and suggests a new approach to increase the stability of electron pair condensates at higher temperatures.","downloadable_attachments":[{"id":43243500,"asset_id":22652408,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":25454076,"first_name":"Philip","last_name":"turner","domain_name":"independent","page_name":"Philipturner8","display_name":"Philip turner","profile_url":"https://independent.academia.edu/Philipturner8?f_ri=34232","photo":"https://0.academia-photos.com/25454076/11783821/13135073/s65_philip.turner.jpg"}],"research_interests":[{"id":317,"name":"Fractal Geometry","url":"https://www.academia.edu/Documents/in/Fractal_Geometry?f_ri=34232","nofollow":true},{"id":3396,"name":"Foundations of Quantum Mechanics","url":"https://www.academia.edu/Documents/in/Foundations_of_Quantum_Mechanics?f_ri=34232","nofollow":true},{"id":3504,"name":"General Relativity","url":"https://www.academia.edu/Documents/in/General_Relativity?f_ri=34232","nofollow":true},{"id":7936,"name":"Quantum Mechanics","url":"https://www.academia.edu/Documents/in/Quantum_Mechanics?f_ri=34232","nofollow":true},{"id":24831,"name":"Fractals","url":"https://www.academia.edu/Documents/in/Fractals?f_ri=34232"},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232"},{"id":179365,"name":"Cuprates","url":"https://www.academia.edu/Documents/in/Cuprates?f_ri=34232"},{"id":213631,"name":"High Temperature Superconductors","url":"https://www.academia.edu/Documents/in/High_Temperature_Superconductors?f_ri=34232"},{"id":730238,"name":"Fractals and Chaos","url":"https://www.academia.edu/Documents/in/Fractals_and_Chaos?f_ri=34232"},{"id":890611,"name":"Fractal Dimension","url":"https://www.academia.edu/Documents/in/Fractal_Dimension?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_873377" data-work_id="873377" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/873377/Raman_scattering_versus_infrared_conductivity_Evidence_for_one_dimensional_conduction_in_La2_xSrxCuO4">Raman scattering versus infrared conductivity: Evidence for one-dimensional conduction in La2-xSrxCuO4</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Raman and infrared (IR) spectra of an underdoped La1.90Sr0.10CuO4 single crystal have been measured as a function of temperature. Both techniques provide unconventional low-energy spectra. The IR conductivity exhibits features peaked at... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_873377" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Raman and infrared (IR) spectra of an underdoped La1.90Sr0.10CuO4 single crystal have been measured as a function of temperature. Both techniques provide unconventional low-energy spectra. The IR conductivity exhibits features peaked at finite frequencies which do not have a counterpart in the Raman response. Below approximately 100 K a transfer of both Raman and IR spectral weight towards lower energies is found and a new component in the Raman response builds up being characterized by a very long lifetime of electrons propagating along the Cu-O bonds.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/873377" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="5167491d43360426e37f2ba08e099293" rel="nofollow" data-download="{"attachment_id":5279393,"asset_id":873377,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/5279393/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="120634" href="https://ethz.academia.edu/AndreaLucarelli">Andrea Lucarelli</a><script data-card-contents-for-user="120634" type="text/json">{"id":120634,"first_name":"Andrea","last_name":"Lucarelli","domain_name":"ethz","page_name":"AndreaLucarelli","display_name":"Andrea Lucarelli","profile_url":"https://ethz.academia.edu/AndreaLucarelli?f_ri=34232","photo":"https://0.academia-photos.com/120634/32392/29769/s65_andrea.lucarelli.jpg"}</script></span></span></li><li class="js-paper-rank-work_873377 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="873377"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 873377, container: ".js-paper-rank-work_873377", }); 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Both techniques provide unconventional low-energy spectra. The IR conductivity exhibits features peaked at finite frequencies which do not have a counterpart in the Raman response. Below approximately 100 K a transfer of both Raman and IR spectral weight towards lower energies is found and a new component in the Raman response builds up being characterized by a very long lifetime of electrons propagating along the Cu-O bonds.\n","downloadable_attachments":[{"id":5279393,"asset_id":873377,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":120634,"first_name":"Andrea","last_name":"Lucarelli","domain_name":"ethz","page_name":"AndreaLucarelli","display_name":"Andrea Lucarelli","profile_url":"https://ethz.academia.edu/AndreaLucarelli?f_ri=34232","photo":"https://0.academia-photos.com/120634/32392/29769/s65_andrea.lucarelli.jpg"}],"research_interests":[{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true},{"id":6649,"name":"Infrared Optics","url":"https://www.academia.edu/Documents/in/Infrared_Optics?f_ri=34232","nofollow":true},{"id":9339,"name":"Raman Spectroscopy","url":"https://www.academia.edu/Documents/in/Raman_Spectroscopy?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":213233,"name":"Optical conductivity","url":"https://www.academia.edu/Documents/in/Optical_conductivity?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_15169721" data-work_id="15169721" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/15169721/Measurements_of_Stationary_Josephson_Current_between_High_Tc_Oxides_as_a_Tool_to_Detect_Charge_Density_Waves">Measurements of Stationary Josephson Current between High-Tc Oxides as a Tool to Detect Charge Density Waves</a></div></div><div class="u-pb4x u-mt3x"></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/15169721" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="98611f2568782bc3e52b0b2ca0050f09" rel="nofollow" data-download="{"attachment_id":38565859,"asset_id":15169721,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/38565859/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="3159343" href="https://iop-kiev.academia.edu/AlexanderGabovich">Alexander M Gabovich</a><script data-card-contents-for-user="3159343" type="text/json">{"id":3159343,"first_name":"Alexander","last_name":"Gabovich","domain_name":"iop-kiev","page_name":"AlexanderGabovich","display_name":"Alexander M Gabovich","profile_url":"https://iop-kiev.academia.edu/AlexanderGabovich?f_ri=34232","photo":"https://0.academia-photos.com/3159343/1074807/1341057/s65_alexander.gabovich.jpg"}</script></span></span></li><li class="js-paper-rank-work_15169721 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="15169721"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 15169721, container: ".js-paper-rank-work_15169721", }); 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But their bulky sizes at lower operating frequencies make them quite inconvenient to be used especially in the frequency range 1-4 GHz, which is the range... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_47574396" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Microwave Cavity Filters are widely used in RF systems for high Q signal filtering. But their bulky sizes at lower operating frequencies make them quite inconvenient to be used especially in the frequency range 1-4 GHz, which is the range of most of the commercial wireless applications. This thesis work aims to enhance the usability of cavity filters in these lower frequency ranges, by exploring a unique reentrant structure for the cavity filter design. The study further explores the use of superconductors in the design to for improve the performance of the filters by reducing the associated losses. After verifying the basic workability of the concept, a coupled reentrant cavity filter design is proposed with an equivalent high Q.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/47574396" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="565ac621e3157c404c6b50fbac8e669e" rel="nofollow" data-download="{"attachment_id":66597651,"asset_id":47574396,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/66597651/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="179016917" href="https://independent.academia.edu/disfort">dirk isfort</a><script data-card-contents-for-user="179016917" type="text/json">{"id":179016917,"first_name":"dirk","last_name":"isfort","domain_name":"independent","page_name":"disfort","display_name":"dirk isfort","profile_url":"https://independent.academia.edu/disfort?f_ri=34232","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_47574396 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="47574396"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 47574396, container: ".js-paper-rank-work_47574396", }); 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$(".js-view-count[data-work-id=47574396]").text(description); $(".js-view-count-work_47574396").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_47574396").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="47574396"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">10</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="56" rel="nofollow" href="https://www.academia.edu/Documents/in/Materials_Engineering">Materials Engineering</a>, <script data-card-contents-for-ri="56" type="text/json">{"id":56,"name":"Materials Engineering","url":"https://www.academia.edu/Documents/in/Materials_Engineering?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="505" rel="nofollow" href="https://www.academia.edu/Documents/in/Condensed_Matter_Physics">Condensed Matter Physics</a>, <script data-card-contents-for-ri="505" type="text/json">{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="34232" rel="nofollow" href="https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY">HIGH TEMPERATURE SUPERCONDUCTIVITY</a>, <script data-card-contents-for-ri="34232" type="text/json">{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="42555" rel="nofollow" href="https://www.academia.edu/Documents/in/Communication_System">Communication System</a><script data-card-contents-for-ri="42555" type="text/json">{"id":42555,"name":"Communication System","url":"https://www.academia.edu/Documents/in/Communication_System?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=47574396]'), work: {"id":47574396,"title":"High Tc superconductor re-entrant cavity filter structures","created_at":"2021-04-23T05:16:14.005-07:00","url":"https://www.academia.edu/47574396/High_Tc_superconductor_re_entrant_cavity_filter_structures?f_ri=34232","dom_id":"work_47574396","summary":"Microwave Cavity Filters are widely used in RF systems for high Q signal filtering. But their bulky sizes at lower operating frequencies make them quite inconvenient to be used especially in the frequency range 1-4 GHz, which is the range of most of the commercial wireless applications. This thesis work aims to enhance the usability of cavity filters in these lower frequency ranges, by exploring a unique reentrant structure for the cavity filter design. The study further explores the use of superconductors in the design to for improve the performance of the filters by reducing the associated losses. After verifying the basic workability of the concept, a coupled reentrant cavity filter design is proposed with an equivalent high Q.","downloadable_attachments":[{"id":66597651,"asset_id":47574396,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":179016917,"first_name":"dirk","last_name":"isfort","domain_name":"independent","page_name":"disfort","display_name":"dirk isfort","profile_url":"https://independent.academia.edu/disfort?f_ri=34232","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":56,"name":"Materials Engineering","url":"https://www.academia.edu/Documents/in/Materials_Engineering?f_ri=34232","nofollow":true},{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true},{"id":42555,"name":"Communication System","url":"https://www.academia.edu/Documents/in/Communication_System?f_ri=34232","nofollow":true},{"id":48458,"name":"High Frequency","url":"https://www.academia.edu/Documents/in/High_Frequency?f_ri=34232"},{"id":103186,"name":"Quality Factor","url":"https://www.academia.edu/Documents/in/Quality_Factor?f_ri=34232"},{"id":125513,"name":"Superconductors","url":"https://www.academia.edu/Documents/in/Superconductors?f_ri=34232"},{"id":993873,"name":"Copper Oxide","url":"https://www.academia.edu/Documents/in/Copper_Oxide?f_ri=34232"},{"id":1237788,"name":"Electrical And Electronic Engineering","url":"https://www.academia.edu/Documents/in/Electrical_And_Electronic_Engineering?f_ri=34232"},{"id":2599525,"name":"present day","url":"https://www.academia.edu/Documents/in/present_day?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_36926102 coauthored" data-work_id="36926102" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/36926102/Ni_Nanoparticle_Added_Ni_x_Cu_0_5_Tl_0_5_Ba_2_Ca_2_Cu_3_O_10_%CE%B4_Superconductor_Composites_and_Their_Enhanced_Flux_Pinning_Characteristics">Ni Nanoparticle-Added Ni x /(Cu 0.5 Tl 0.5 )Ba 2 Ca 2 Cu 3 O 10-δ Superconductor Composites and Their Enhanced Flux Pinning Characteristics</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Ni nanoparticle-added Ni x /(Cu 0.5 Tl 0.5)Ba 2 Ca 2 Cu 3 O 10-δ superconductor composites are synthesized at normal pressure by two-step solid-state reaction method. The idea for adding ferromagnetic nanoparticles was to create... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_36926102" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Ni nanoparticle-added Ni x /(Cu 0.5 Tl 0.5)Ba 2 Ca 2 Cu 3 O 10-δ superconductor composites are synthesized at normal pressure by two-step solid-state reaction method. The idea for adding ferromagnetic nanoparticles was to create artificial pinning centers at grain boundaries. The samples have shown orthorhombic crystal structure in which the cell parameters increase with an increase in the added concentration of Ni nanoparticles. This shows that due to the higher reactivity, Ni nanoparticles partially diffuse into the unit cell of (Cu 0.5 Tl 0.5)Ba 2 Ca 2 Cu 3 O 10-δ superconductors. This also indicates as an evidence of the occupancy of these nanoparticles at grain boundaries. A metallic variation of resistivity from room temperature down to the onset of superconductivity is a typical feature of these samples with T c (R = 0) varying between 92 and 94 K. The magnitude of diamagnetism is significantly enhanced in 7 and 10% nanoparticle-added samples. The enhanced magnetiza-tion of ferromagnetic nanoparticles at reduced temperature plays a vital role in reducing the diamagnetism of nanosu-perconductor composites. The softening of apical oxygen modes of type Cu(1)–O A –Cu(2) has confirmed the diffusion of Ni nanoparticles into the unit cell of the final compound. The excess conductivity analyses of conductivity data have shown that the values of B c (0), B c1 , and J c are enhanced with the addition of Ni nanoparticles in the final compound. Variation of superconducting properties was attributed to pair breaking due to spin scattering across these ferromagnetic Ni nanoparticles. This shows that added Ni nanoparticles act as efficient pinning centers, which is also confirmed by the suppression of the London penetration depth. Keywords Ni x /(Cu 0.5 Tl 0.5)Ba 2 Ca 2 Cu 3 O 10-δ composite superconductors · Excess conductivity analysis · Enhancement of B c (0), B c1 , and J c · Enhancement of flux pinning · Suppression of London penetration depth</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/36926102" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="bdf186a0c8df4fbf58cb15aba59a17b4" rel="nofollow" data-download="{"attachment_id":56876279,"asset_id":36926102,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/56876279/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="61517273" href="https://johnjanovy.academia.edu/SyedQamarAbbasShah">Syed Qamar Abbas Shah</a><script data-card-contents-for-user="61517273" type="text/json">{"id":61517273,"first_name":"Syed Qamar Abbas","last_name":"Shah","domain_name":"johnjanovy","page_name":"SyedQamarAbbasShah","display_name":"Syed Qamar Abbas Shah","profile_url":"https://johnjanovy.academia.edu/SyedQamarAbbasShah?f_ri=34232","photo":"https://0.academia-photos.com/61517273/16412021/19773261/s65_syed_qamar_abbas.shah.jpg"}</script></span></span><span class="u-displayInlineBlock InlineList-item-text"> and <span class="u-textDecorationUnderline u-clickable InlineList-item-text js-work-more-authors-36926102">+1</span><div class="hidden js-additional-users-36926102"><div><span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a href="https://independent.academia.edu/NawazishKhan1">Nawazish Khan</a></span></div></div></span><script>(function(){ var popoverSettings = { el: $('.js-work-more-authors-36926102'), placement: 'bottom', hide_delay: 200, html: true, content: function(){ return $('.js-additional-users-36926102').html(); 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container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_36926102 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="36926102"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 36926102; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=36926102]").text(description); $(".js-view-count-work_36926102").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_36926102").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="36926102"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">7</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="2306" rel="nofollow" href="https://www.academia.edu/Documents/in/Synthesis_of_nanoparticles">Synthesis of nanoparticles</a>, <script data-card-contents-for-ri="2306" type="text/json">{"id":2306,"name":"Synthesis of nanoparticles","url":"https://www.academia.edu/Documents/in/Synthesis_of_nanoparticles?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="6469" rel="nofollow" href="https://www.academia.edu/Documents/in/Superconductivity">Superconductivity</a>, <script data-card-contents-for-ri="6469" type="text/json">{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="13621" rel="nofollow" href="https://www.academia.edu/Documents/in/Nanoparticles">Nanoparticles</a>, <script data-card-contents-for-ri="13621" type="text/json">{"id":13621,"name":"Nanoparticles","url":"https://www.academia.edu/Documents/in/Nanoparticles?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="27080" rel="nofollow" href="https://www.academia.edu/Documents/in/Vortex_dynamics">Vortex dynamics</a><script data-card-contents-for-ri="27080" type="text/json">{"id":27080,"name":"Vortex dynamics","url":"https://www.academia.edu/Documents/in/Vortex_dynamics?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=36926102]'), work: {"id":36926102,"title":"Ni Nanoparticle-Added Ni x /(Cu 0.5 Tl 0.5 )Ba 2 Ca 2 Cu 3 O 10-δ Superconductor Composites and Their Enhanced Flux Pinning Characteristics","created_at":"2018-06-26T23:57:05.043-07:00","url":"https://www.academia.edu/36926102/Ni_Nanoparticle_Added_Ni_x_Cu_0_5_Tl_0_5_Ba_2_Ca_2_Cu_3_O_10_%CE%B4_Superconductor_Composites_and_Their_Enhanced_Flux_Pinning_Characteristics?f_ri=34232","dom_id":"work_36926102","summary":"Ni nanoparticle-added Ni x /(Cu 0.5 Tl 0.5)Ba 2 Ca 2 Cu 3 O 10-δ superconductor composites are synthesized at normal pressure by two-step solid-state reaction method. The idea for adding ferromagnetic nanoparticles was to create artificial pinning centers at grain boundaries. The samples have shown orthorhombic crystal structure in which the cell parameters increase with an increase in the added concentration of Ni nanoparticles. This shows that due to the higher reactivity, Ni nanoparticles partially diffuse into the unit cell of (Cu 0.5 Tl 0.5)Ba 2 Ca 2 Cu 3 O 10-δ superconductors. This also indicates as an evidence of the occupancy of these nanoparticles at grain boundaries. A metallic variation of resistivity from room temperature down to the onset of superconductivity is a typical feature of these samples with T c (R = 0) varying between 92 and 94 K. The magnitude of diamagnetism is significantly enhanced in 7 and 10% nanoparticle-added samples. The enhanced magnetiza-tion of ferromagnetic nanoparticles at reduced temperature plays a vital role in reducing the diamagnetism of nanosu-perconductor composites. The softening of apical oxygen modes of type Cu(1)–O A –Cu(2) has confirmed the diffusion of Ni nanoparticles into the unit cell of the final compound. The excess conductivity analyses of conductivity data have shown that the values of B c (0), B c1 , and J c are enhanced with the addition of Ni nanoparticles in the final compound. Variation of superconducting properties was attributed to pair breaking due to spin scattering across these ferromagnetic Ni nanoparticles. This shows that added Ni nanoparticles act as efficient pinning centers, which is also confirmed by the suppression of the London penetration depth. Keywords Ni x /(Cu 0.5 Tl 0.5)Ba 2 Ca 2 Cu 3 O 10-δ composite superconductors · Excess conductivity analysis · Enhancement of B c (0), B c1 , and J c · Enhancement of flux pinning · Suppression of London penetration depth","downloadable_attachments":[{"id":56876279,"asset_id":36926102,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":61517273,"first_name":"Syed Qamar Abbas","last_name":"Shah","domain_name":"johnjanovy","page_name":"SyedQamarAbbasShah","display_name":"Syed Qamar Abbas Shah","profile_url":"https://johnjanovy.academia.edu/SyedQamarAbbasShah?f_ri=34232","photo":"https://0.academia-photos.com/61517273/16412021/19773261/s65_syed_qamar_abbas.shah.jpg"},{"id":42785405,"first_name":"Nawazish","last_name":"Khan","domain_name":"independent","page_name":"NawazishKhan1","display_name":"Nawazish Khan","profile_url":"https://independent.academia.edu/NawazishKhan1?f_ri=34232","photo":"https://0.academia-photos.com/42785405/159794180/149468426/s65_nawazish.khan.jpg"}],"research_interests":[{"id":2306,"name":"Synthesis of nanoparticles","url":"https://www.academia.edu/Documents/in/Synthesis_of_nanoparticles?f_ri=34232","nofollow":true},{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232","nofollow":true},{"id":13621,"name":"Nanoparticles","url":"https://www.academia.edu/Documents/in/Nanoparticles?f_ri=34232","nofollow":true},{"id":27080,"name":"Vortex dynamics","url":"https://www.academia.edu/Documents/in/Vortex_dynamics?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232"},{"id":125513,"name":"Superconductors","url":"https://www.academia.edu/Documents/in/Superconductors?f_ri=34232"},{"id":1199295,"name":"Flux Pinning","url":"https://www.academia.edu/Documents/in/Flux_Pinning?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_35470521" data-work_id="35470521" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/35470521/IMPORTANT_UPDATE_On_the_Trail_of_a_Secret_Pentagon_UFO_Program_The_New_York_Timespdf_pdf">IMPORTANT UPDATE On the Trail of a Secret Pentagon UFO Program The New York Timespdf.pdf</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest">Memorandum for the record on recent release of US Navy video on unidentified aerial vehicles and the physics that may explain them.</div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/35470521" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="9acc1c34954a5867e4c083c917fae1ce" rel="nofollow" data-download="{"attachment_id":55332946,"asset_id":35470521,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/55332946/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="690537" href="https://cornell.academia.edu/JackSarfatti">Jack Sarfatti</a><script data-card-contents-for-user="690537" type="text/json">{"id":690537,"first_name":"Jack","last_name":"Sarfatti","domain_name":"cornell","page_name":"JackSarfatti","display_name":"Jack Sarfatti","profile_url":"https://cornell.academia.edu/JackSarfatti?f_ri=34232","photo":"https://0.academia-photos.com/690537/870624/163601433/s65_jack.sarfatti.jpg"}</script></span></span></li><li class="js-paper-rank-work_35470521 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="35470521"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 35470521, container: ".js-paper-rank-work_35470521", }); });</script></li><li class="js-percentile-work_35470521 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 35470521; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = 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style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="35470521"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">9</a>  </div><span class="InlineList-item-text u-textTruncate u-pl9x"><a class="InlineList-item-text" data-has-card-for-ri="498" rel="nofollow" href="https://www.academia.edu/Documents/in/Physics">Physics</a>, <script data-card-contents-for-ri="498" type="text/json">{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="3504" rel="nofollow" href="https://www.academia.edu/Documents/in/General_Relativity">General Relativity</a>, <script data-card-contents-for-ri="3504" type="text/json">{"id":3504,"name":"General Relativity","url":"https://www.academia.edu/Documents/in/General_Relativity?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="6650" rel="nofollow" href="https://www.academia.edu/Documents/in/Electromagnetic_metamaterials">Electromagnetic metamaterials</a>, <script data-card-contents-for-ri="6650" type="text/json">{"id":6650,"name":"Electromagnetic metamaterials","url":"https://www.academia.edu/Documents/in/Electromagnetic_metamaterials?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="10018" rel="nofollow" href="https://www.academia.edu/Documents/in/Metamaterials">Metamaterials</a><script data-card-contents-for-ri="10018" type="text/json">{"id":10018,"name":"Metamaterials","url":"https://www.academia.edu/Documents/in/Metamaterials?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=35470521]'), work: {"id":35470521,"title":"IMPORTANT UPDATE On the Trail of a Secret Pentagon UFO Program The New York Timespdf.pdf","created_at":"2017-12-19T11:47:18.658-08:00","url":"https://www.academia.edu/35470521/IMPORTANT_UPDATE_On_the_Trail_of_a_Secret_Pentagon_UFO_Program_The_New_York_Timespdf_pdf?f_ri=34232","dom_id":"work_35470521","summary":"Memorandum for the record on recent release of US Navy video on unidentified aerial vehicles and the physics that may explain them.","downloadable_attachments":[{"id":55332946,"asset_id":35470521,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":690537,"first_name":"Jack","last_name":"Sarfatti","domain_name":"cornell","page_name":"JackSarfatti","display_name":"Jack Sarfatti","profile_url":"https://cornell.academia.edu/JackSarfatti?f_ri=34232","photo":"https://0.academia-photos.com/690537/870624/163601433/s65_jack.sarfatti.jpg"}],"research_interests":[{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics?f_ri=34232","nofollow":true},{"id":3504,"name":"General Relativity","url":"https://www.academia.edu/Documents/in/General_Relativity?f_ri=34232","nofollow":true},{"id":6650,"name":"Electromagnetic metamaterials","url":"https://www.academia.edu/Documents/in/Electromagnetic_metamaterials?f_ri=34232","nofollow":true},{"id":10018,"name":"Metamaterials","url":"https://www.academia.edu/Documents/in/Metamaterials?f_ri=34232","nofollow":true},{"id":12100,"name":"Aviation","url":"https://www.academia.edu/Documents/in/Aviation?f_ri=34232"},{"id":23985,"name":"Space Propulsion","url":"https://www.academia.edu/Documents/in/Space_Propulsion?f_ri=34232"},{"id":24557,"name":"Propulsion","url":"https://www.academia.edu/Documents/in/Propulsion?f_ri=34232"},{"id":31260,"name":"Bose Einstein Condensation","url":"https://www.academia.edu/Documents/in/Bose_Einstein_Condensation?f_ri=34232"},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_32954632 coauthored" data-work_id="32954632" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/32954632/Design_and_Simulation_of_SMES_System_Using_YBCO_Tapes_for_Direct_Drive_Wave_Energy_Converters">Design and Simulation of SMES System Using YBCO Tapes for Direct Drive Wave Energy Converters</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">The ocean represents a huge energy reservoir since waves can be exploited to generate clean and renewable electricity; however, a hybrid energy storage system is needed to smooth the fluctuation. In this paper a hybrid energy storage... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_32954632" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">The ocean represents a huge energy reservoir since waves can be exploited to generate clean and renewable electricity; however, a hybrid energy storage system is needed to smooth the fluctuation. In this paper a hybrid energy storage system using a superconducting magnetic energy system (SMES) and Li-ion battery is proposed. The SMES is designed using Yttrium Barium Copper Oxide (YBCO) tapes, which store 60 kJ electrical energy. The magnet component of the SMES is designed using global optimization algorithm. Mechanical stress, coupled with electromagnetic field, is calculated using COMSOL and Matlab. A cooling system is presented and a suitable refrigerator is chosen to maintain a cold working temperature taking into account four heat sources. Then a microgrid system of direct drive linear wave energy converters is designed. The interface circuit connecting the generator and storage system is given. The result reveals that the fluctuated power from direct drive linear wave energy converters is smoothed by the hybrid energy storage system. The maximum power of the wave energy converter is 10 kW.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/32954632" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="9aa0c3f4f0d318de8046bf76bea68fb4" rel="nofollow" data-download="{"attachment_id":53082707,"asset_id":32954632,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/53082707/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="34312033" href="https://independent.academia.edu/TCoombs1">T. Coombs</a><script data-card-contents-for-user="34312033" type="text/json">{"id":34312033,"first_name":"T.","last_name":"Coombs","domain_name":"independent","page_name":"TCoombs1","display_name":"T. Coombs","profile_url":"https://independent.academia.edu/TCoombs1?f_ri=34232","photo":"/images/s65_no_pic.png"}</script></span></span><span class="u-displayInlineBlock InlineList-item-text"> and <span class="u-textDecorationUnderline u-clickable InlineList-item-text js-work-more-authors-32954632">+1</span><div class="hidden js-additional-users-32954632"><div><span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a href="https://independent.academia.edu/JiahuiZhu2">Jiahui Zhu</a></span></div></div></span><script>(function(){ var popoverSettings = { el: $('.js-work-more-authors-32954632'), placement: 'bottom', hide_delay: 200, html: true, content: function(){ return $('.js-additional-users-32954632').html(); } } new HoverPopover(popoverSettings); })();</script></li><li class="js-paper-rank-work_32954632 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="32954632"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 32954632, container: ".js-paper-rank-work_32954632", }); });</script></li><li class="js-percentile-work_32954632 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 32954632; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_32954632"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_32954632 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="32954632"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 32954632; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=32954632]").text(description); $(".js-view-count-work_32954632").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_32954632").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="32954632"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">14</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="49" rel="nofollow" href="https://www.academia.edu/Documents/in/Electrical_Engineering">Electrical Engineering</a>, <script data-card-contents-for-ri="49" type="text/json">{"id":49,"name":"Electrical Engineering","url":"https://www.academia.edu/Documents/in/Electrical_Engineering?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="56" rel="nofollow" href="https://www.academia.edu/Documents/in/Materials_Engineering">Materials Engineering</a>, <script data-card-contents-for-ri="56" type="text/json">{"id":56,"name":"Materials Engineering","url":"https://www.academia.edu/Documents/in/Materials_Engineering?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="505" rel="nofollow" href="https://www.academia.edu/Documents/in/Condensed_Matter_Physics">Condensed Matter Physics</a>, <script data-card-contents-for-ri="505" type="text/json">{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="2738" rel="nofollow" href="https://www.academia.edu/Documents/in/Renewable_Energy">Renewable Energy</a><script data-card-contents-for-ri="2738" type="text/json">{"id":2738,"name":"Renewable Energy","url":"https://www.academia.edu/Documents/in/Renewable_Energy?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=32954632]'), work: {"id":32954632,"title":"Design and Simulation of SMES System Using YBCO Tapes for Direct Drive Wave Energy Converters","created_at":"2017-05-11T04:49:51.111-07:00","url":"https://www.academia.edu/32954632/Design_and_Simulation_of_SMES_System_Using_YBCO_Tapes_for_Direct_Drive_Wave_Energy_Converters?f_ri=34232","dom_id":"work_32954632","summary":"The ocean represents a huge energy reservoir since waves can be exploited to generate clean and renewable electricity; however, a hybrid energy storage system is needed to smooth the fluctuation. In this paper a hybrid energy storage system using a superconducting magnetic energy system (SMES) and Li-ion battery is proposed. The SMES is designed using Yttrium Barium Copper Oxide (YBCO) tapes, which store 60 kJ electrical energy. The magnet component of the SMES is designed using global optimization algorithm. Mechanical stress, coupled with electromagnetic field, is calculated using COMSOL and Matlab. A cooling system is presented and a suitable refrigerator is chosen to maintain a cold working temperature taking into account four heat sources. Then a microgrid system of direct drive linear wave energy converters is designed. The interface circuit connecting the generator and storage system is given. The result reveals that the fluctuated power from direct drive linear wave energy converters is smoothed by the hybrid energy storage system. The maximum power of the wave energy converter is 10 kW.","downloadable_attachments":[{"id":53082707,"asset_id":32954632,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":34312033,"first_name":"T.","last_name":"Coombs","domain_name":"independent","page_name":"TCoombs1","display_name":"T. Coombs","profile_url":"https://independent.academia.edu/TCoombs1?f_ri=34232","photo":"/images/s65_no_pic.png"},{"id":64269011,"first_name":"Jiahui","last_name":"Zhu","domain_name":"independent","page_name":"JiahuiZhu2","display_name":"Jiahui Zhu","profile_url":"https://independent.academia.edu/JiahuiZhu2?f_ri=34232","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":49,"name":"Electrical Engineering","url":"https://www.academia.edu/Documents/in/Electrical_Engineering?f_ri=34232","nofollow":true},{"id":56,"name":"Materials Engineering","url":"https://www.academia.edu/Documents/in/Materials_Engineering?f_ri=34232","nofollow":true},{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics?f_ri=34232","nofollow":true},{"id":2738,"name":"Renewable Energy","url":"https://www.academia.edu/Documents/in/Renewable_Energy?f_ri=34232","nofollow":true},{"id":3172,"name":"Wave Energy","url":"https://www.academia.edu/Documents/in/Wave_Energy?f_ri=34232"},{"id":6469,"name":"Superconductivity","url":"https://www.academia.edu/Documents/in/Superconductivity?f_ri=34232"},{"id":12719,"name":"Electric Energy Storage","url":"https://www.academia.edu/Documents/in/Electric_Energy_Storage?f_ri=34232"},{"id":16330,"name":"Energy Storage (in Engineering)","url":"https://www.academia.edu/Documents/in/Energy_Storage_in_Engineering_?f_ri=34232"},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232"},{"id":34819,"name":"Electric Power Systems","url":"https://www.academia.edu/Documents/in/Electric_Power_Systems?f_ri=34232"},{"id":63240,"name":"Applied Superconductivity","url":"https://www.academia.edu/Documents/in/Applied_Superconductivity?f_ri=34232"},{"id":125513,"name":"Superconductors","url":"https://www.academia.edu/Documents/in/Superconductors?f_ri=34232"},{"id":213631,"name":"High Temperature Superconductors","url":"https://www.academia.edu/Documents/in/High_Temperature_Superconductors?f_ri=34232"},{"id":1237788,"name":"Electrical And Electronic Engineering","url":"https://www.academia.edu/Documents/in/Electrical_And_Electronic_Engineering?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_7724209" data-work_id="7724209" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/7724209/Electrochemical_approaches_to_the_production_of_graphene_flakes_and_their_potential_applications">Electrochemical approaches to the production of graphene flakes and their potential applications</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Graphene (GN) has many beneficial properties that encourage wide applications. Various manufacturing procedures are detailed in the literature but most are unable to produce GN flakes in bulk and usually result in toxic discharges. These... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_7724209" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Graphene (GN) has many beneficial properties that encourage wide applications. Various manufacturing procedures are detailed in the literature but most are unable to produce GN flakes in bulk and usually result in toxic discharges. These techniques are also time-consuming and involve operations at high temperatures. A 'greener', simpler and a one-step synthesis of the material may be realised by electrochemical oxidation (or reduction) of the graphite host leading to intercalation of ions from the electrolyte (which may be aqueous, organic or an ionic liquid) followed by electrochemical exfoliation. Single- or multi-layered GN flakes can easily be produced in short periods of time, typically within 30 min. This paper reviews the state-of-the-art methods reported in the literature regarding electrochemical synthesis of GN flakes as well as their properties (determined via sophisticated analytical methods such as AFM, TEM, SEM or Raman spectroscopy). This is followed by a discussion on the applications of electrochemically prepared GN flakes. Challenges and opportunities are briefly considered leading to the conclusion that the cathodic intercalation of lithium ions into graphite can produce the highest yield (>70%) of pristine GN flakes in organic electrolytes. Future work is recommended with ternary eutectic melts as electrolytes. © 2012 Elsevier Ltd. All rights reserved. <br /> <br /><a href="http://ac.els-cdn.com/S0008622312009219/1-s2.0-S0008622312009219-main.pdf?_tid=83fff34a-0ca1-11e4-aae5-00000aab0f26&acdnat=1405485037_e682436f6620bf78eff4d2a366977e36" rel="nofollow">http://ac.els-cdn.com/S0008622312009219/1-s2.0-S0008622312009219-main.pdf?_tid=83fff34a-0ca1-11e4-aae5-00000aab0f26&acdnat=1405485037_e682436f6620bf78eff4d2a366977e36</a>  <br /><a href="http://www.sciencedirect.com/science/article/pii/S0008622312009219" rel="nofollow">http://www.sciencedirect.com/science/article/pii/S0008622312009219</a></div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/7724209" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="389f4c967e38f78ee8340d20325ef674" rel="nofollow" data-download="{"attachment_id":34248536,"asset_id":7724209,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/34248536/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="13958389" href="https://malaya.academia.edu/MohdAliHashim">Mohd Ali Hashim</a><script data-card-contents-for-user="13958389" type="text/json">{"id":13958389,"first_name":"Mohd Ali","last_name":"Hashim","domain_name":"malaya","page_name":"MohdAliHashim","display_name":"Mohd Ali Hashim","profile_url":"https://malaya.academia.edu/MohdAliHashim?f_ri=34232","photo":"https://0.academia-photos.com/13958389/4018074/4690936/s65_mohd_ali.hashim.jpg"}</script></span></span></li><li class="js-paper-rank-work_7724209 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="7724209"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 7724209, container: ".js-paper-rank-work_7724209", }); });</script></li><li class="js-percentile-work_7724209 InlineList-item InlineList-item--bordered hidden u-tcGrayDark"><span class="percentile-widget hidden"><span class="u-mr2x percentile-widget" style="display: none">•</span><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 7724209; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-percentile-work_7724209"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></li><li class="js-view-count-work_7724209 InlineList-item InlineList-item--bordered hidden"><div><span><span class="js-view-count view-count u-mr2x" data-work-id="7724209"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 7724209; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=7724209]").text(description); $(".js-view-count-work_7724209").attr('title', description).tooltip(); }); });</script></span><script>$(function() { $(".js-view-count-work_7724209").removeClass('hidden') })</script></div></li><li class="InlineList-item u-positionRelative" style="max-width: 250px"><div class="u-positionAbsolute" data-has-card-for-ri-list="7724209"><i class="fa fa-tag InlineList-item-icon u-positionRelative"></i>  <a class="InlineList-item-text u-positionRelative">17</a>  </div><span class="InlineList-item-text u-textTruncate u-pl10x"><a class="InlineList-item-text" data-has-card-for-ri="9339" rel="nofollow" href="https://www.academia.edu/Documents/in/Raman_Spectroscopy">Raman Spectroscopy</a>, <script data-card-contents-for-ri="9339" type="text/json">{"id":9339,"name":"Raman Spectroscopy","url":"https://www.academia.edu/Documents/in/Raman_Spectroscopy?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="11541" rel="nofollow" href="https://www.academia.edu/Documents/in/Graphene">Graphene</a>, <script data-card-contents-for-ri="11541" type="text/json">{"id":11541,"name":"Graphene","url":"https://www.academia.edu/Documents/in/Graphene?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="19927" rel="nofollow" href="https://www.academia.edu/Documents/in/Analytical_Method_Development">Analytical Method Development</a>, <script data-card-contents-for-ri="19927" type="text/json">{"id":19927,"name":"Analytical Method Development","url":"https://www.academia.edu/Documents/in/Analytical_Method_Development?f_ri=34232","nofollow":true}</script><a class="InlineList-item-text" data-has-card-for-ri="33003" rel="nofollow" href="https://www.academia.edu/Documents/in/Ionic_Liquids">Ionic Liquids</a><script data-card-contents-for-ri="33003" type="text/json">{"id":33003,"name":"Ionic Liquids","url":"https://www.academia.edu/Documents/in/Ionic_Liquids?f_ri=34232","nofollow":true}</script></span></li><script>(function(){ if (true) { new Aedu.ResearchInterestListCard({ el: $('*[data-has-card-for-ri-list=7724209]'), work: {"id":7724209,"title":"Electrochemical approaches to the production of graphene flakes and their potential applications","created_at":"2014-07-20T11:11:39.780-07:00","url":"https://www.academia.edu/7724209/Electrochemical_approaches_to_the_production_of_graphene_flakes_and_their_potential_applications?f_ri=34232","dom_id":"work_7724209","summary":"Graphene (GN) has many beneficial properties that encourage wide applications. Various manufacturing procedures are detailed in the literature but most are unable to produce GN flakes in bulk and usually result in toxic discharges. These techniques are also time-consuming and involve operations at high temperatures. A 'greener', simpler and a one-step synthesis of the material may be realised by electrochemical oxidation (or reduction) of the graphite host leading to intercalation of ions from the electrolyte (which may be aqueous, organic or an ionic liquid) followed by electrochemical exfoliation. Single- or multi-layered GN flakes can easily be produced in short periods of time, typically within 30 min. This paper reviews the state-of-the-art methods reported in the literature regarding electrochemical synthesis of GN flakes as well as their properties (determined via sophisticated analytical methods such as AFM, TEM, SEM or Raman spectroscopy). This is followed by a discussion on the applications of electrochemically prepared GN flakes. Challenges and opportunities are briefly considered leading to the conclusion that the cathodic intercalation of lithium ions into graphite can produce the highest yield (\u003e70%) of pristine GN flakes in organic electrolytes. Future work is recommended with ternary eutectic melts as electrolytes. © 2012 Elsevier Ltd. All rights reserved.\r\n\r\nhttp://ac.els-cdn.com/S0008622312009219/1-s2.0-S0008622312009219-main.pdf?_tid=83fff34a-0ca1-11e4-aae5-00000aab0f26\u0026acdnat=1405485037_e682436f6620bf78eff4d2a366977e36 \r\nhttp://www.sciencedirect.com/science/article/pii/S0008622312009219 ","downloadable_attachments":[{"id":34248536,"asset_id":7724209,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":13958389,"first_name":"Mohd Ali","last_name":"Hashim","domain_name":"malaya","page_name":"MohdAliHashim","display_name":"Mohd Ali Hashim","profile_url":"https://malaya.academia.edu/MohdAliHashim?f_ri=34232","photo":"https://0.academia-photos.com/13958389/4018074/4690936/s65_mohd_ali.hashim.jpg"}],"research_interests":[{"id":9339,"name":"Raman Spectroscopy","url":"https://www.academia.edu/Documents/in/Raman_Spectroscopy?f_ri=34232","nofollow":true},{"id":11541,"name":"Graphene","url":"https://www.academia.edu/Documents/in/Graphene?f_ri=34232","nofollow":true},{"id":19927,"name":"Analytical Method Development","url":"https://www.academia.edu/Documents/in/Analytical_Method_Development?f_ri=34232","nofollow":true},{"id":33003,"name":"Ionic Liquids","url":"https://www.academia.edu/Documents/in/Ionic_Liquids?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232"},{"id":72820,"name":"Graphite","url":"https://www.academia.edu/Documents/in/Graphite?f_ri=34232"},{"id":75498,"name":"AFM","url":"https://www.academia.edu/Documents/in/AFM?f_ri=34232"},{"id":112010,"name":"Potential Applications of Cyanobacteria","url":"https://www.academia.edu/Documents/in/Potential_Applications_of_Cyanobacteria?f_ri=34232"},{"id":562068,"name":"Polymer Electrolytes","url":"https://www.academia.edu/Documents/in/Polymer_Electrolytes?f_ri=34232"},{"id":796597,"name":"Synthesis of Tin Oxide Nano Particles by Electrochemical Reduction Methode","url":"https://www.academia.edu/Documents/in/Synthesis_of_Tin_Oxide_Nano_Particles_by_Electrochemical_Reduction_Methode?f_ri=34232"},{"id":830479,"name":"Electric Discharges","url":"https://www.academia.edu/Documents/in/Electric_Discharges?f_ri=34232"},{"id":965113,"name":"Multi layered","url":"https://www.academia.edu/Documents/in/Multi_layered?f_ri=34232"},{"id":1063424,"name":"Organic Electrolyte","url":"https://www.academia.edu/Documents/in/Organic_Electrolyte?f_ri=34232"},{"id":1294513,"name":"Electrochemical Oxidation","url":"https://www.academia.edu/Documents/in/Electrochemical_Oxidation?f_ri=34232"},{"id":1455526,"name":"Manufacturing Procedure","url":"https://www.academia.edu/Documents/in/Manufacturing_Procedure?f_ri=34232"},{"id":1455527,"name":"Short Periods","url":"https://www.academia.edu/Documents/in/Short_Periods?f_ri=34232"},{"id":1455529,"name":"Ternary Eutectics","url":"https://www.academia.edu/Documents/in/Ternary_Eutectics?f_ri=34232"}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_4220470" data-work_id="4220470" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/4220470/PHYSICAL_REVIEW_B_86_024523_2012_Topological_superconducting_phase_in_the_vicinity_of_ferromagnetic_phases">PHYSICAL REVIEW B 86, 024523 (2012) Topological superconducting phase in the vicinity of ferromagnetic phases</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">Through the study of concrete models we establish a strong tie between topological superconductivity and ferromagnetic spin correlations. Our result can be used as a guideline for the search for topological superconductors whose pairing... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_4220470" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">Through the study of concrete models we establish a strong tie between topological superconductivity and ferromagnetic spin correlations. Our result can be used as a guideline for the search for topological superconductors whose pairing symmetry is invariant under time reversal. The results are obtained by the functional renormalization group method.</div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/4220470" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="515f70c911882b69a1f562bc8d16638a" rel="nofollow" data-download="{"attachment_id":31708384,"asset_id":4220470,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/31708384/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="5108412" href="https://nanjing.academia.edu/YuanXiang">Yuan Xiang</a><script data-card-contents-for-user="5108412" type="text/json">{"id":5108412,"first_name":"Yuan","last_name":"Xiang","domain_name":"nanjing","page_name":"YuanXiang","display_name":"Yuan Xiang","profile_url":"https://nanjing.academia.edu/YuanXiang?f_ri=34232","photo":"/images/s65_no_pic.png"}</script></span></span></li><li class="js-paper-rank-work_4220470 InlineList-item InlineList-item--bordered hidden"><span class="js-paper-rank-view hidden u-tcGrayDark" data-paper-rank-work-id="4220470"><i class="u-m1x fa fa-bar-chart"></i><strong class="js-paper-rank"></strong></span><script>$(function() { new Works.PaperRankView({ workId: 4220470, container: ".js-paper-rank-work_4220470", }); 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Our result can be used as a guideline for the search for topological superconductors whose pairing symmetry is invariant under time reversal. The results are obtained by the functional renormalization group method.","downloadable_attachments":[{"id":31708384,"asset_id":4220470,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":5108412,"first_name":"Yuan","last_name":"Xiang","domain_name":"nanjing","page_name":"YuanXiang","display_name":"Yuan Xiang","profile_url":"https://nanjing.academia.edu/YuanXiang?f_ri=34232","photo":"/images/s65_no_pic.png"}],"research_interests":[{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232","nofollow":true}]}, }) } })();</script></ul></li></ul></div></div><div class="u-borderBottom1 u-borderColorGrayLighter"><div class="clearfix u-pv7x u-mb0x js-work-card work_3971039" data-work_id="3971039" itemscope="itemscope" itemtype="https://schema.org/ScholarlyArticle"><div class="header"><div class="title u-fontSerif u-fs22 u-lineHeight1_3"><a class="u-tcGrayDarkest js-work-link" href="https://www.academia.edu/3971039/Effects_of_bismuth_oxide_on_the_sinterability_of_hydroxyapatite">Effects of bismuth oxide on the sinterability of hydroxyapatite</a></div></div><div class="u-pb4x u-mt3x"><div class="summary u-fs14 u-fw300 u-lineHeight1_5 u-tcGrayDarkest"><div class="summarized">The sinterability of Bi(2)O(3)-doped hydroxyapatite (HA) has been studied and compared with the undoped HA. Varying amounts of Bi(2)O(3) ranging from 0.05 wt% to 1.0 wt% were mixed with the HA. The study revealed that most sintered... <a class="more_link u-tcGrayDark u-linkUnstyled" data-container=".work_3971039" data-show=".complete" data-hide=".summarized" data-more-link-behavior="true" href="#">more</a></div><div class="complete hidden">The sinterability of Bi(2)O(3)-doped hydroxyapatite (HA) has been studied and compared with the undoped HA. Varying amounts of Bi(2)O(3) ranging from 0.05 wt% to 1.0 wt% were mixed with the HA. The study revealed that most sintered samples composed of the HA phase except for compacts containing 0.3, 0.5 and 1.0 wt% Bi(2)O(3) and when sintered above 1100 degrees C, 1000 degrees C and 950 degrees C, respectively. In general, the addition of 0.5 wt% Bi(2)O(3) was identified as the optimum amount to promote densification as well as to improve the mechanical properties of sintered HA at low temperature of 1000 degrees C. Throughout the sintering regime, the highest value of relative bulk density of 98.7% was obtained for 0.5 wt% Bi(2)O(3)-doped HA when sintered at 1000 degrees C. A maximum Young's modulus of 119.2 GPa was measured for 0.1 wt% Bi(2)O(3)-doped HA when sintered at 1150 degrees C. Additionally, the ceramic was able to achieve highest hardness of 6.08 GPa and fracture toughness of 1.21 MPa m(1/2) at sintering temperature of 1000 degrees C. <br /> <br /><a href="http://ac.els-cdn.com/S0272884210003974/1-s2.0-S0272884210003974-main.pdf?_tid=791dbb38-e777-11e2-b24b-00000aab0f01&acdnat=1373251289_895d761089b3e72d2cac363f0410f248" rel="nofollow">http://ac.els-cdn.com/S0272884210003974/1-s2.0-S0272884210003974-main.pdf?_tid=791dbb38-e777-11e2-b24b-00000aab0f01&acdnat=1373251289_895d761089b3e72d2cac363f0410f248</a></div></div></div><ul class="InlineList u-ph0x u-fs13"><li class="InlineList-item logged_in_only"><div class="share_on_academia_work_button"><a class="academia_share Button Button--inverseBlue Button--sm js-bookmark-button" data-academia-share="Work/3971039" data-share-source="work_strip" data-spinner="small_white_hide_contents"><i class="fa fa-plus"></i><span class="work-strip-link-text u-ml1x" data-content="button_text">Bookmark</span></a></div></li><li class="InlineList-item"><div class="download"><a id="09089e4d26a6bb769b8fd3b69ffdc57c" rel="nofollow" data-download="{"attachment_id":31536864,"asset_id":3971039,"asset_type":"Work","always_allow_download":false,"track":null,"button_location":"work_strip","source":null,"hide_modal":null}" class="Button Button--sm Button--inverseGreen js-download-button prompt_button doc_download" href="https://www.academia.edu/attachments/31536864/download_file?st=MTczOTgzMjMyNSw4LjIyMi4yMDguMTQ2&s=work_strip"><i class="fa fa-arrow-circle-o-down fa-lg"></i><span class="u-textUppercase u-ml1x" data-content="button_text">Download</span></a></div></li><li class="InlineList-item"><ul class="InlineList InlineList--bordered u-ph0x"><li class="InlineList-item InlineList-item--bordered"><span class="InlineList-item-text">by <span itemscope="itemscope" itemprop="author" itemtype="https://schema.org/Person"><a class="u-tcGrayDark u-fw700" data-has-card-for-user="3364553" href="https://malaya.academia.edu/SRamesh">S. 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Varying amounts of Bi(2)O(3) ranging from 0.05 wt% to 1.0 wt% were mixed with the HA. The study revealed that most sintered samples composed of the HA phase except for compacts containing 0.3, 0.5 and 1.0 wt% Bi(2)O(3) and when sintered above 1100 degrees C, 1000 degrees C and 950 degrees C, respectively. In general, the addition of 0.5 wt% Bi(2)O(3) was identified as the optimum amount to promote densification as well as to improve the mechanical properties of sintered HA at low temperature of 1000 degrees C. Throughout the sintering regime, the highest value of relative bulk density of 98.7% was obtained for 0.5 wt% Bi(2)O(3)-doped HA when sintered at 1000 degrees C. A maximum Young's modulus of 119.2 GPa was measured for 0.1 wt% Bi(2)O(3)-doped HA when sintered at 1150 degrees C. Additionally, the ceramic was able to achieve highest hardness of 6.08 GPa and fracture toughness of 1.21 MPa m(1/2) at sintering temperature of 1000 degrees C.\r\n\r\nhttp://ac.els-cdn.com/S0272884210003974/1-s2.0-S0272884210003974-main.pdf?_tid=791dbb38-e777-11e2-b24b-00000aab0f01\u0026acdnat=1373251289_895d761089b3e72d2cac363f0410f248 ","downloadable_attachments":[{"id":31536864,"asset_id":3971039,"asset_type":"Work","always_allow_download":false}],"ordered_authors":[{"id":3364553,"first_name":"S.","last_name":"Ramesh","domain_name":"malaya","page_name":"SRamesh","display_name":"S. Ramesh","profile_url":"https://malaya.academia.edu/SRamesh?f_ri=34232","photo":"https://0.academia-photos.com/3364553/1130534/2406579/s65_ramesh_singh.kuldip_singh.jpg"}],"research_interests":[{"id":4495,"name":"Mechanical Properties of Ceramics","url":"https://www.academia.edu/Documents/in/Mechanical_Properties_of_Ceramics?f_ri=34232","nofollow":true},{"id":7293,"name":"Market Microstructure","url":"https://www.academia.edu/Documents/in/Market_Microstructure?f_ri=34232","nofollow":true},{"id":21831,"name":"Natural Fibre Composites","url":"https://www.academia.edu/Documents/in/Natural_Fibre_Composites?f_ri=34232","nofollow":true},{"id":23047,"name":"Fracture Mechanics","url":"https://www.academia.edu/Documents/in/Fracture_Mechanics?f_ri=34232","nofollow":true},{"id":34232,"name":"HIGH TEMPERATURE SUPERCONDUCTIVITY","url":"https://www.academia.edu/Documents/in/HIGH_TEMPERATURE_SUPERCONDUCTIVITY?f_ri=34232"},{"id":41117,"name":"Tissue Engineering: Hard Tissue Engineering (Bone 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