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</a></div></div></div></div><div class="right-panel-container"><div class="user-content-wrapper"><div class="uploads-container" id="social-redesign-work-container"><div class="upload-header"><h2 class="ds2-5-heading-sans-serif-xs">Uploads</h2></div><div class="documents-container backbone-social-profile-documents" style="width: 100%;"><div class="u-taCenter"></div><div class="profile--tab_content_container js-tab-pane tab-pane active" id="all"><div class="profile--tab_heading_container js-section-heading" data-section="Papers" id="Papers"><h3 class="profile--tab_heading_container">Papers by Abdelmajid Ainane</h3></div><div class="js-work-strip profile--work_container" data-work-id="78774878"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/78774878/Negatively_Charged_Exciton_Inside_Type_I_and_Reversed_Type_I_Core_Shell_Nanodots_A_Comparative_Study"><img alt="Research paper thumbnail of Negatively Charged Exciton Inside Type-I and Reversed Type-I Core/Shell Nanodots: A Comparative Study" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/78774878/Negatively_Charged_Exciton_Inside_Type_I_and_Reversed_Type_I_Core_Shell_Nanodots_A_Comparative_Study">Negatively Charged Exciton Inside Type-I and Reversed Type-I Core/Shell Nanodots: A Comparative Study</a></div><div class="wp-workCard_item"><span>SSRN Electronic Journal</span><span>, 2022</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span 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$('.js-work-strip[data-work-id=78774878]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":78774878,"title":"Negatively Charged Exciton Inside Type-I and Reversed Type-I Core/Shell Nanodots: A Comparative Study","internal_url":"https://www.academia.edu/78774878/Negatively_Charged_Exciton_Inside_Type_I_and_Reversed_Type_I_Core_Shell_Nanodots_A_Comparative_Study","owner_id":14512644,"coauthors_can_edit":true,"owner":{"id":14512644,"first_name":"Abdelmajid","middle_initials":null,"last_name":"Ainane","page_name":"AbdelmajidAinane","domain_name":"independent","created_at":"2014-07-30T06:43:57.378-07:00","display_name":"Abdelmajid Ainane","url":"https://independent.academia.edu/AbdelmajidAinane"},"attachments":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="78774877"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/78774877/Magnetic_properties_of_a_diluted_transverse_spin_Ising_film"><img alt="Research paper thumbnail of Magnetic properties of a diluted transverse spin- Ising film" class="work-thumbnail" src="https://attachments.academia-assets.com/85701207/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/78774877/Magnetic_properties_of_a_diluted_transverse_spin_Ising_film">Magnetic properties of a diluted transverse spin- Ising film</a></div><div class="wp-workCard_item"><span>Physica A: Statistical Mechanics and its Applications</span><span>, 1999</span></div><div 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dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="78774876"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/78774876/Modeling_the_influence_of_the_seeding_layer_on_the_transition_behavior_of_a_ferroelectric_thin_film"><img alt="Research paper thumbnail of Modeling the influence of the seeding layer on the transition behavior of a ferroelectric thin film" class="work-thumbnail" src="https://attachments.academia-assets.com/85701208/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/78774876/Modeling_the_influence_of_the_seeding_layer_on_the_transition_behavior_of_a_ferroelectric_thin_film">Modeling the influence of the seeding layer on the transition behavior of a ferroelectric thin film</a></div><div class="wp-workCard_item"><span>Thin Solid Films</span><span>, 2011</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The transition properties of a ferroelectric thin film with seeding layers were studied using the...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The transition properties of a ferroelectric thin film with seeding layers were studied using the effective field theory with a probability distribution technique that accounts for the self-spin correlation functions. The effect of interaction parameters for the seeding layer on the phase diagram was also examined. We calculated the critical temperature and the polarization of the ferroelectric thin film for different seeding layer structures. We found that the seeding layer can greatly increase the Curie temperature and the polarization.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="2d0e5a0e02ebb962094fb12803f8d6d9" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":85701208,"asset_id":78774876,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/85701208/download_file?s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="78774876"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="78774876"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 78774876; 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</script> <div class="js-work-strip profile--work_container" data-work-id="72902669"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902669/2D_Janus_and_non_Janus_diamanes_with_an_in_plane_negative_Poissons_ratio_for_energy_applications"><img alt="Research paper thumbnail of 2D Janus and non-Janus diamanes with an in-plane negative Poisson's ratio for energy applications" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902669/2D_Janus_and_non_Janus_diamanes_with_an_in_plane_negative_Poissons_ratio_for_energy_applications">2D Janus and non-Janus diamanes with an in-plane negative Poisson's ratio for energy applications</a></div><div class="wp-workCard_item"><span>Materials Today Advances</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902669"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902669"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902669; 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</script> <div class="js-work-strip profile--work_container" data-work-id="72902660"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902660/Dielectric_Properties_and_Hysteresis_Loops_of_the_Bilayer_Ising_Model"><img alt="Research paper thumbnail of Dielectric Properties and Hysteresis Loops of the Bilayer Ising Model" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902660/Dielectric_Properties_and_Hysteresis_Loops_of_the_Bilayer_Ising_Model">Dielectric Properties and Hysteresis Loops of the Bilayer Ising Model</a></div><div class="wp-workCard_item"><span>Chinese Journal of Physics</span><span>, 2009</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The hysteresis loops, susceptibility, and pyroelectric coefficient of a ferroelectric or ferroele...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The hysteresis loops, susceptibility, and pyroelectric coefficient of a ferroelectric or ferroelectric bilayer system consisting of two monolayers (A and B) with different spins (S(subscript A)=σ=1/2 and S(subscript B)=S=3/2) in the presence of the crystal field in the monolayer B have been studied. Within an unusual mean-field theory based on the probability distribution technique that accounts for the self spin correlation functions, we discuss the effects of the external longitudinal electric field on the polarization, susceptibility, and pyroelectric coefficient of the cubic lattice. We show that by a choice of the temperature the hysteresis loops can be varied over a very wide range.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902660"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902660"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902660; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902660]").text(description); 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</script> <div class="js-work-strip profile--work_container" data-work-id="72902648"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902648/The_Dielectric_Properties_of_the_KH2PO4_KD2H2PO4_Superlattice"><img alt="Research paper thumbnail of The Dielectric Properties of the KH2PO4/KD2H2PO4 Superlattice" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902648/The_Dielectric_Properties_of_the_KH2PO4_KD2H2PO4_Superlattice">The Dielectric Properties of the KH2PO4/KD2H2PO4 Superlattice</a></div><div class="wp-workCard_item"><span>Chinese Journal of Physics</span><span>, 2007</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Using the effective field theory with a probability distribution technique, we apply the Ising mo...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Using the effective field theory with a probability distribution technique, we apply the Ising model in a transverse field to analyse the properties of a KH2PO4/KD2H2PO4 superlattice. The on-site polarization and dielectric susceptibility, their mean values, the susceptibility, and the macroscopic pyroelectric coefficient are calculated for possible comparison with experimental data. We found for thick layer superlattices two peaks in the mean dielectric susceptibility and pyroelectric coefficient, as they had two phase transitions, whereas thin-layer superlattices show a one-peak behavior.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902648"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902648"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902648; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902648]").text(description); $(".js-view-count[data-work-id=72902648]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902648; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902648']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=72902648]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":72902648,"title":"The Dielectric Properties of the KH2PO4/KD2H2PO4 Superlattice","internal_url":"https://www.academia.edu/72902648/The_Dielectric_Properties_of_the_KH2PO4_KD2H2PO4_Superlattice","owner_id":14512644,"coauthors_can_edit":true,"owner":{"id":14512644,"first_name":"Abdelmajid","middle_initials":null,"last_name":"Ainane","page_name":"AbdelmajidAinane","domain_name":"independent","created_at":"2014-07-30T06:43:57.378-07:00","display_name":"Abdelmajid Ainane","url":"https://independent.academia.edu/AbdelmajidAinane"},"attachments":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902644"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/72902644/The_influence_of_layer_defect_in_the_Ferroelectric_films"><img alt="Research paper thumbnail of The influence of layer defect in the Ferroelectric films" class="work-thumbnail" src="https://attachments.academia-assets.com/81641418/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/72902644/The_influence_of_layer_defect_in_the_Ferroelectric_films">The influence of layer defect in the Ferroelectric films</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Using the modified transverse Ising model, and the effective field theory based on the probabilit...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Using the modified transverse Ising model, and the effective field theory based on the probability distribution technique, the phase transition temperature, the polarization and susceptibility for ferroelectric thin films with structural defects are studied. It is shown that the defect layers in ferroelectric thin films can induce strong increase or decrease of the critical temperature of ferroelectric phase transition due to different exchange interactions in the defect layers. The obtained results are in qualitative agreement with experimental data for thin ferroelectric film with different thickness.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="4ab9a810a375df3c2dd04aabbaaa6863" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":81641418,"asset_id":72902644,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/81641418/download_file?s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902644"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902644"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902644; 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window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902641]").text(description); $(".js-view-count[data-work-id=72902641]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902641; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902641']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=72902641]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":72902641,"title":"Phase transitions in a transverse spin-1/2 ising ferroelectric superlattice","internal_url":"https://www.academia.edu/72902641/Phase_transitions_in_a_transverse_spin_1_2_ising_ferroelectric_superlattice","owner_id":14512644,"coauthors_can_edit":true,"owner":{"id":14512644,"first_name":"Abdelmajid","middle_initials":null,"last_name":"Ainane","page_name":"AbdelmajidAinane","domain_name":"independent","created_at":"2014-07-30T06:43:57.378-07:00","display_name":"Abdelmajid Ainane","url":"https://independent.academia.edu/AbdelmajidAinane"},"attachments":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902638"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902638/Phase_Diagrams_of_the_Site_Diluted_Spin_i_Ising_Film_in_a_Transverse_Field"><img alt="Research paper thumbnail of Phase Diagrams of the Site-Diluted Spin-i Ising Film in a Transverse Field" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902638/Phase_Diagrams_of_the_Site_Diluted_Spin_i_Ising_Film_in_a_Transverse_Field">Phase Diagrams of the Site-Diluted Spin-i Ising Film in a Transverse Field</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Within the framework of the effective field theory, with a probability distribution technique tha...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Within the framework of the effective field theory, with a probability distribution technique that accounts for the single-site spin correlations, we examine the critical behavior of a diluted spin-1/2 Ising film. The critical temperature of the system is studied as a function of the thickness of the film, the concentration of magnetic atoms, the strength of the transverse field and the couplings. It is shown that for the ratio of the surface couplings to the bulk ones R = Js/J less than a critical value R,, the critical temperature of the film Tc/J is smaller than the bulk critical temperature Tc^B/J and for R ≥ Rc, Tc/J is larger than the bulk critical temperature Tc^B/J and Tc^S/J of the corresponding semi-infinite system. As the film thickness L is increased further Tc/J increases for R ≤ Rc (decreases for R 2 R,) and approaches asymptotically for large values of L the bulk critical temperature Tc^B/J (the surface critical temperature Tc^S/J) of the corresponding semi-infinite s...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902638"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902638"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902638; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902617"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902617/Hysteresis_Behavior_and_Pyroelectric_Properties_of_Multi_Surface_Ferroelectric_Thin_Films"><img alt="Research paper thumbnail of Hysteresis Behavior and Pyroelectric Properties of Multi-Surface Ferroelectric Thin Films" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902617/Hysteresis_Behavior_and_Pyroelectric_Properties_of_Multi_Surface_Ferroelectric_Thin_Films">Hysteresis Behavior and Pyroelectric Properties of Multi-Surface Ferroelectric Thin Films</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Using the transverse Ising model, we investigate the dielectric properties and the hysteresis beh...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Using the transverse Ising model, we investigate the dielectric properties and the hysteresis behavior of multi-surface ferroelectric (MSF) thin films in the framework of the effective field theory based on the probability distribution technique that accounts for the self-spin correlation functions. The effects of the exchange interactions and the transverse field on the longitudinal and the transverse polarizations, the dielectric susceptibility, the pyroelectric coefficient, and the hysteresis loops are studied. A number of interesting phenomena have been found.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902617"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902617"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902617; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902617]").text(description); $(".js-view-count[data-work-id=72902617]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902617; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902617']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=72902617]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":72902617,"title":"Hysteresis Behavior and Pyroelectric Properties of Multi-Surface Ferroelectric Thin Films","internal_url":"https://www.academia.edu/72902617/Hysteresis_Behavior_and_Pyroelectric_Properties_of_Multi_Surface_Ferroelectric_Thin_Films","owner_id":14512644,"coauthors_can_edit":true,"owner":{"id":14512644,"first_name":"Abdelmajid","middle_initials":null,"last_name":"Ainane","page_name":"AbdelmajidAinane","domain_name":"independent","created_at":"2014-07-30T06:43:57.378-07:00","display_name":"Abdelmajid Ainane","url":"https://independent.academia.edu/AbdelmajidAinane"},"attachments":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902613"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902613/Some_Magnetic_Properties_of_the_Amorphous_Transverse_Spin_1_2_Ising_System"><img alt="Research paper thumbnail of Some Magnetic Properties of the Amorphous Transverse Spin-1/2 Ising System" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902613/Some_Magnetic_Properties_of_the_Amorphous_Transverse_Spin_1_2_Ising_System">Some Magnetic Properties of the Amorphous Transverse Spin-1/2 Ising System</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Some Magnetic Properties of the Amorphous Transverse Spin-12 Ising System I. Essaoudi,1 F. Dujard...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Some Magnetic Properties of the Amorphous Transverse Spin-12 Ising System I. Essaoudi,1 F. Dujardin,2 A. Ainane,1, 3, ∗ M. Saber,1, 3, 4 and J. Gonzalez4 Laboratoire de Physique des Matériaux et Modélisation des Systémes (LP2MS), Unité Associée au CNRST, Physics Department, Faculty of Sciences, University of Moulay Ismail, B.P. 11201, Meknes, Morocco Laboratoire de Physique des Milieux Denses (LPMD) Institut de Chimie, Physique et Matériaux (ICPM), 1 Bd. Arago, 57070, Metz, France Max-Planck-Institut für Physik Complexer Systeme, Nöthnitzer Str. 38 D-01187 Dresden, Germany Basque Country University, Material Physics Dept. (UPV/EHU) Paseo Manuel de Lardizabal, 3, San Sebastian, 20018, Spain (Received May 22, 2009)</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902613"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902613"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902613; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902613]").text(description); $(".js-view-count[data-work-id=72902613]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902613; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902613']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=72902613]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":72902613,"title":"Some Magnetic Properties of the Amorphous Transverse Spin-1/2 Ising System","internal_url":"https://www.academia.edu/72902613/Some_Magnetic_Properties_of_the_Amorphous_Transverse_Spin_1_2_Ising_System","owner_id":14512644,"coauthors_can_edit":true,"owner":{"id":14512644,"first_name":"Abdelmajid","middle_initials":null,"last_name":"Ainane","page_name":"AbdelmajidAinane","domain_name":"independent","created_at":"2014-07-30T06:43:57.378-07:00","display_name":"Abdelmajid Ainane","url":"https://independent.academia.edu/AbdelmajidAinane"},"attachments":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902607"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902607/A_Theoretical_Study_of_Hysteresis_Behaviors_of_2D_Mixed_Spin_1_2_1_Ising_Nanopaticles"><img alt="Research paper thumbnail of A Theoretical Study of Hysteresis Behaviors of 2D Mixed Spin-(1/2,1)Ising Nanopaticles" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902607/A_Theoretical_Study_of_Hysteresis_Behaviors_of_2D_Mixed_Spin_1_2_1_Ising_Nanopaticles">A Theoretical Study of Hysteresis Behaviors of 2D Mixed Spin-(1/2,1)Ising Nanopaticles</a></div><div class="wp-workCard_item"><span>2018 6th International Renewable and Sustainable Energy Conference (IRSEC)</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The EffectiveField Theory with correlations (EFT) based on the probability distribution is used t...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The EffectiveField Theory with correlations (EFT) based on the probability distribution is used to investigate the magnetic hysteresis behaviors of both hexagonal and square 2D nanoparticles consisting of a ferromagnetic spin-1/2 core and a ferromagnetic spin-l shell. The system parameters such as the ferrimagnetic exchange core/shell interaction, the surface shell exchange coupling and the reduced temperatureare examined on the magnetic hysteresis behaviors. Some interesting results have been found such as multiple hysteresis loop behaviors.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902607"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902607"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902607; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902607]").text(description); $(".js-view-count[data-work-id=72902607]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902607; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902607']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=72902607]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":72902607,"title":"A Theoretical Study of Hysteresis Behaviors of 2D Mixed Spin-(1/2,1)Ising Nanopaticles","internal_url":"https://www.academia.edu/72902607/A_Theoretical_Study_of_Hysteresis_Behaviors_of_2D_Mixed_Spin_1_2_1_Ising_Nanopaticles","owner_id":14512644,"coauthors_can_edit":true,"owner":{"id":14512644,"first_name":"Abdelmajid","middle_initials":null,"last_name":"Ainane","page_name":"AbdelmajidAinane","domain_name":"independent","created_at":"2014-07-30T06:43:57.378-07:00","display_name":"Abdelmajid Ainane","url":"https://independent.academia.edu/AbdelmajidAinane"},"attachments":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902601"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902601/Rational_Design_of_2D_h_BAs_Monolayer_as_Advanced_Sulfur_Host_for_High_Energy_Density_Li_S_Batteries"><img alt="Research paper thumbnail of Rational Design of 2D h-BAs Monolayer as Advanced Sulfur Host for High Energy Density Li–S Batteries" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902601/Rational_Design_of_2D_h_BAs_Monolayer_as_Advanced_Sulfur_Host_for_High_Energy_Density_Li_S_Batteries">Rational Design of 2D h-BAs Monolayer as Advanced Sulfur Host for High Energy Density Li–S Batteries</a></div><div class="wp-workCard_item"><span>ACS Applied Energy Materials</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The emergence of compact lithium-sulfur (Li-S) batteries with improved performances is becoming o...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The emergence of compact lithium-sulfur (Li-S) batteries with improved performances is becoming one of the most desirable aspects of future energy technologies. Beyond Li-ion batteries, Li-S is of great relevance to follow as it adapts to the specificity of each application. It is among the most suitable elements for high-performance energy storage systems, given its high theoretical capacity (1674 mA h g(-1)) and energy density (2600 W h kg(-1)) relative to Li-ion batteries (300 W h kg(-1)). Nevertheless, the high-cell polarization and the shuttle effect constitute an enormous challenge toward the concrete applications of Li-S batteries. In the framework of this work, density functional theory calculations have been carried out to analyze the potential of h-BAs nanosheets as a promising host material for Li-S batteries. Binding and electronic characteristics of lithium polysulfides (LiPSs) adsorbed on h-BAs surface have been explored. Reported findings highlight the potential of the hBAs monolayer as a moderate host material, given that the binding energies of different LiPSs vary from 0.47 to 3.55 eV. More detailed analysis of the complex binding mechanisms is carried out by investigating the components of van der Waals physical/chemical interactions. The defected surface of the h-BAs monolayer has optimum binding energies with LiPSs for Li-S batteries. All these findings provide valuable insights into the binding and electronic characteristics of the h-BAs monolayer as a moderate host material for Li-S batteries.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902601"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902601"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902601; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902601]").text(description); $(".js-view-count[data-work-id=72902601]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902601; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902601']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); 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</script> <div class="js-work-strip profile--work_container" data-work-id="72902598"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902598/Electronic_optical_and_thermoelectric_properties_of_two_dimensional_pentagonal_SiGeC4_nanosheet_for_photovoltaic_applications_First_principles_calculations"><img alt="Research paper thumbnail of Electronic, optical and thermoelectric properties of two-dimensional pentagonal SiGeC4 nanosheet for photovoltaic applications: First-principles calculations" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902598/Electronic_optical_and_thermoelectric_properties_of_two_dimensional_pentagonal_SiGeC4_nanosheet_for_photovoltaic_applications_First_principles_calculations">Electronic, optical and thermoelectric properties of two-dimensional pentagonal SiGeC4 nanosheet for photovoltaic applications: First-principles calculations</a></div><div class="wp-workCard_item"><span>Superlattices and Microstructures</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902598"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902598"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902598; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902598]").text(description); $(".js-view-count[data-work-id=72902598]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902598; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902598']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902592"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902592/Thermodynamics_and_kinetics_of_2D_g_GeC_monolayer_as_an_anode_materials_for_Li_Na_ion_batteries"><img alt="Research paper thumbnail of Thermodynamics and kinetics of 2D g-GeC monolayer as an anode materials for Li/Na-ion batteries" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902592/Thermodynamics_and_kinetics_of_2D_g_GeC_monolayer_as_an_anode_materials_for_Li_Na_ion_batteries">Thermodynamics and kinetics of 2D g-GeC monolayer as an anode materials for Li/Na-ion batteries</a></div><div class="wp-workCard_item"><span>Journal of Power Sources</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902592"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902592"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902592; 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</script> <div class="js-work-strip profile--work_container" data-work-id="72902586"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902586/Computational_identification_of_efficient_2D_Aluminium_chalcogenides_monolayers_for_optoelectronics_and_photocatalysts_applications"><img alt="Research paper thumbnail of Computational identification of efficient 2D Aluminium chalcogenides monolayers for optoelectronics and photocatalysts applications" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902586/Computational_identification_of_efficient_2D_Aluminium_chalcogenides_monolayers_for_optoelectronics_and_photocatalysts_applications">Computational identification of efficient 2D Aluminium chalcogenides monolayers for optoelectronics and photocatalysts applications</a></div><div class="wp-workCard_item"><span>Applied Surface Science</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902586"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902586"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902586; 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</script> <div class="js-work-strip profile--work_container" data-work-id="78774877"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/78774877/Magnetic_properties_of_a_diluted_transverse_spin_Ising_film"><img alt="Research paper thumbnail of Magnetic properties of a diluted transverse spin- Ising film" class="work-thumbnail" src="https://attachments.academia-assets.com/85701207/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/78774877/Magnetic_properties_of_a_diluted_transverse_spin_Ising_film">Magnetic properties of a diluted transverse spin- Ising film</a></div><div class="wp-workCard_item"><span>Physica A: Statistical Mechanics and its Applications</span><span>, 1999</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="d622f24a0996396b7c2c4eed54d4cde6" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":85701207,"asset_id":78774877,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/85701207/download_file?s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="78774877"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="78774877"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 78774877; 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The effect of interaction parameters for the seeding layer on the phase diagram was also examined. We calculated the critical temperature and the polarization of the ferroelectric thin film for different seeding layer structures. We found that the seeding layer can greatly increase the Curie temperature and the polarization.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="2d0e5a0e02ebb962094fb12803f8d6d9" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":85701208,"asset_id":78774876,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/85701208/download_file?s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="78774876"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="78774876"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 78774876; 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Within an unusual mean-field theory based on the probability distribution technique that accounts for the self spin correlation functions, we discuss the effects of the external longitudinal electric field on the polarization, susceptibility, and pyroelectric coefficient of the cubic lattice. 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</script> <div class="js-work-strip profile--work_container" data-work-id="72902648"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902648/The_Dielectric_Properties_of_the_KH2PO4_KD2H2PO4_Superlattice"><img alt="Research paper thumbnail of The Dielectric Properties of the KH2PO4/KD2H2PO4 Superlattice" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902648/The_Dielectric_Properties_of_the_KH2PO4_KD2H2PO4_Superlattice">The Dielectric Properties of the KH2PO4/KD2H2PO4 Superlattice</a></div><div class="wp-workCard_item"><span>Chinese Journal of Physics</span><span>, 2007</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Using the effective field theory with a probability distribution technique, we apply the Ising mo...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Using the effective field theory with a probability distribution technique, we apply the Ising model in a transverse field to analyse the properties of a KH2PO4/KD2H2PO4 superlattice. The on-site polarization and dielectric susceptibility, their mean values, the susceptibility, and the macroscopic pyroelectric coefficient are calculated for possible comparison with experimental data. We found for thick layer superlattices two peaks in the mean dielectric susceptibility and pyroelectric coefficient, as they had two phase transitions, whereas thin-layer superlattices show a one-peak behavior.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902648"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902648"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902648; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902648]").text(description); $(".js-view-count[data-work-id=72902648]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902648; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902648']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=72902648]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":72902648,"title":"The Dielectric Properties of the KH2PO4/KD2H2PO4 Superlattice","internal_url":"https://www.academia.edu/72902648/The_Dielectric_Properties_of_the_KH2PO4_KD2H2PO4_Superlattice","owner_id":14512644,"coauthors_can_edit":true,"owner":{"id":14512644,"first_name":"Abdelmajid","middle_initials":null,"last_name":"Ainane","page_name":"AbdelmajidAinane","domain_name":"independent","created_at":"2014-07-30T06:43:57.378-07:00","display_name":"Abdelmajid Ainane","url":"https://independent.academia.edu/AbdelmajidAinane"},"attachments":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902644"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/72902644/The_influence_of_layer_defect_in_the_Ferroelectric_films"><img alt="Research paper thumbnail of The influence of layer defect in the Ferroelectric films" class="work-thumbnail" src="https://attachments.academia-assets.com/81641418/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/72902644/The_influence_of_layer_defect_in_the_Ferroelectric_films">The influence of layer defect in the Ferroelectric films</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Using the modified transverse Ising model, and the effective field theory based on the probabilit...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Using the modified transverse Ising model, and the effective field theory based on the probability distribution technique, the phase transition temperature, the polarization and susceptibility for ferroelectric thin films with structural defects are studied. It is shown that the defect layers in ferroelectric thin films can induce strong increase or decrease of the critical temperature of ferroelectric phase transition due to different exchange interactions in the defect layers. The obtained results are in qualitative agreement with experimental data for thin ferroelectric film with different thickness.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="4ab9a810a375df3c2dd04aabbaaa6863" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":81641418,"asset_id":72902644,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/81641418/download_file?s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902644"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902644"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902644; 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902641"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902641/Phase_transitions_in_a_transverse_spin_1_2_ising_ferroelectric_superlattice"><img alt="Research paper thumbnail of Phase transitions in a transverse spin-1/2 ising ferroelectric superlattice" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902641/Phase_transitions_in_a_transverse_spin_1_2_ising_ferroelectric_superlattice">Phase transitions in a transverse spin-1/2 ising ferroelectric superlattice</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">ABSTRACT</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902641"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902641"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902641; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902641]").text(description); $(".js-view-count[data-work-id=72902641]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902641; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902641']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=72902641]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":72902641,"title":"Phase transitions in a transverse spin-1/2 ising ferroelectric superlattice","internal_url":"https://www.academia.edu/72902641/Phase_transitions_in_a_transverse_spin_1_2_ising_ferroelectric_superlattice","owner_id":14512644,"coauthors_can_edit":true,"owner":{"id":14512644,"first_name":"Abdelmajid","middle_initials":null,"last_name":"Ainane","page_name":"AbdelmajidAinane","domain_name":"independent","created_at":"2014-07-30T06:43:57.378-07:00","display_name":"Abdelmajid Ainane","url":"https://independent.academia.edu/AbdelmajidAinane"},"attachments":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902638"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902638/Phase_Diagrams_of_the_Site_Diluted_Spin_i_Ising_Film_in_a_Transverse_Field"><img alt="Research paper thumbnail of Phase Diagrams of the Site-Diluted Spin-i Ising Film in a Transverse Field" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902638/Phase_Diagrams_of_the_Site_Diluted_Spin_i_Ising_Film_in_a_Transverse_Field">Phase Diagrams of the Site-Diluted Spin-i Ising Film in a Transverse Field</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Within the framework of the effective field theory, with a probability distribution technique tha...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Within the framework of the effective field theory, with a probability distribution technique that accounts for the single-site spin correlations, we examine the critical behavior of a diluted spin-1/2 Ising film. The critical temperature of the system is studied as a function of the thickness of the film, the concentration of magnetic atoms, the strength of the transverse field and the couplings. It is shown that for the ratio of the surface couplings to the bulk ones R = Js/J less than a critical value R,, the critical temperature of the film Tc/J is smaller than the bulk critical temperature Tc^B/J and for R ≥ Rc, Tc/J is larger than the bulk critical temperature Tc^B/J and Tc^S/J of the corresponding semi-infinite system. As the film thickness L is increased further Tc/J increases for R ≤ Rc (decreases for R 2 R,) and approaches asymptotically for large values of L the bulk critical temperature Tc^B/J (the surface critical temperature Tc^S/J) of the corresponding semi-infinite s...</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902638"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902638"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902638; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902638]").text(description); $(".js-view-count[data-work-id=72902638]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902638; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902638']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=72902638]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":72902638,"title":"Phase Diagrams of the Site-Diluted Spin-i Ising Film in a Transverse Field","internal_url":"https://www.academia.edu/72902638/Phase_Diagrams_of_the_Site_Diluted_Spin_i_Ising_Film_in_a_Transverse_Field","owner_id":14512644,"coauthors_can_edit":true,"owner":{"id":14512644,"first_name":"Abdelmajid","middle_initials":null,"last_name":"Ainane","page_name":"AbdelmajidAinane","domain_name":"independent","created_at":"2014-07-30T06:43:57.378-07:00","display_name":"Abdelmajid Ainane","url":"https://independent.academia.edu/AbdelmajidAinane"},"attachments":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902633"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" href="https://www.academia.edu/72902633/Effective_Critical_Exponent_of_the_Magnetization_in_Ferromagnetic_Ising_Films_with_Amorphous_Surfaces"><img alt="Research paper thumbnail of Effective Critical Exponent of the Magnetization in Ferromagnetic Ising Films with Amorphous Surfaces" class="work-thumbnail" src="https://attachments.academia-assets.com/83898134/thumbnails/1.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" href="https://www.academia.edu/72902633/Effective_Critical_Exponent_of_the_Magnetization_in_Ferromagnetic_Ising_Films_with_Amorphous_Surfaces">Effective Critical Exponent of the Magnetization in Ferromagnetic Ising Films with Amorphous Surfaces</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Technische Universita¨t Chemnitz, 09107 Chemnitz, Germany(Received March 4, 2006)The characterist...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Technische Universita¨t Chemnitz, 09107 Chemnitz, Germany(Received March 4, 2006)The characteristic inﬂuence of the exchange interactions and amorphization at the surfaceon the critical behavior of a ferromagnetic Ising ﬁlm is examined, by the use of eﬀective ﬁeldtheory with a probability distribution technique that accounts for the self spin correlations.Depending on the ratio of the surface exchange interactions to the bulk ones, R = J</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="4f73809e7b925c6491a92b20f22031db" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":83898134,"asset_id":72902633,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/83898134/download_file?s=profile"><span><i class="fa fa-arrow-down"></i></span><span>Download</span></a><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902633"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902633"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902633; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902633]").text(description); $(".js-view-count[data-work-id=72902633]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902633; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902633']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (true){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); 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$(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902617"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902617/Hysteresis_Behavior_and_Pyroelectric_Properties_of_Multi_Surface_Ferroelectric_Thin_Films"><img alt="Research paper thumbnail of Hysteresis Behavior and Pyroelectric Properties of Multi-Surface Ferroelectric Thin Films" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902617/Hysteresis_Behavior_and_Pyroelectric_Properties_of_Multi_Surface_Ferroelectric_Thin_Films">Hysteresis Behavior and Pyroelectric Properties of Multi-Surface Ferroelectric Thin Films</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Using the transverse Ising model, we investigate the dielectric properties and the hysteresis beh...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Using the transverse Ising model, we investigate the dielectric properties and the hysteresis behavior of multi-surface ferroelectric (MSF) thin films in the framework of the effective field theory based on the probability distribution technique that accounts for the self-spin correlation functions. The effects of the exchange interactions and the transverse field on the longitudinal and the transverse polarizations, the dielectric susceptibility, the pyroelectric coefficient, and the hysteresis loops are studied. A number of interesting phenomena have been found.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902617"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902617"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902617; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902617]").text(description); $(".js-view-count[data-work-id=72902617]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902617; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902617']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=72902617]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":72902617,"title":"Hysteresis Behavior and Pyroelectric Properties of Multi-Surface Ferroelectric Thin Films","internal_url":"https://www.academia.edu/72902617/Hysteresis_Behavior_and_Pyroelectric_Properties_of_Multi_Surface_Ferroelectric_Thin_Films","owner_id":14512644,"coauthors_can_edit":true,"owner":{"id":14512644,"first_name":"Abdelmajid","middle_initials":null,"last_name":"Ainane","page_name":"AbdelmajidAinane","domain_name":"independent","created_at":"2014-07-30T06:43:57.378-07:00","display_name":"Abdelmajid Ainane","url":"https://independent.academia.edu/AbdelmajidAinane"},"attachments":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902613"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902613/Some_Magnetic_Properties_of_the_Amorphous_Transverse_Spin_1_2_Ising_System"><img alt="Research paper thumbnail of Some Magnetic Properties of the Amorphous Transverse Spin-1/2 Ising System" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902613/Some_Magnetic_Properties_of_the_Amorphous_Transverse_Spin_1_2_Ising_System">Some Magnetic Properties of the Amorphous Transverse Spin-1/2 Ising System</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Some Magnetic Properties of the Amorphous Transverse Spin-12 Ising System I. Essaoudi,1 F. Dujard...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">Some Magnetic Properties of the Amorphous Transverse Spin-12 Ising System I. Essaoudi,1 F. Dujardin,2 A. Ainane,1, 3, ∗ M. Saber,1, 3, 4 and J. Gonzalez4 Laboratoire de Physique des Matériaux et Modélisation des Systémes (LP2MS), Unité Associée au CNRST, Physics Department, Faculty of Sciences, University of Moulay Ismail, B.P. 11201, Meknes, Morocco Laboratoire de Physique des Milieux Denses (LPMD) Institut de Chimie, Physique et Matériaux (ICPM), 1 Bd. Arago, 57070, Metz, France Max-Planck-Institut für Physik Complexer Systeme, Nöthnitzer Str. 38 D-01187 Dresden, Germany Basque Country University, Material Physics Dept. (UPV/EHU) Paseo Manuel de Lardizabal, 3, San Sebastian, 20018, Spain (Received May 22, 2009)</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902613"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902613"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902613; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902613]").text(description); $(".js-view-count[data-work-id=72902613]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902613; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902613']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=72902613]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":72902613,"title":"Some Magnetic Properties of the Amorphous Transverse Spin-1/2 Ising System","internal_url":"https://www.academia.edu/72902613/Some_Magnetic_Properties_of_the_Amorphous_Transverse_Spin_1_2_Ising_System","owner_id":14512644,"coauthors_can_edit":true,"owner":{"id":14512644,"first_name":"Abdelmajid","middle_initials":null,"last_name":"Ainane","page_name":"AbdelmajidAinane","domain_name":"independent","created_at":"2014-07-30T06:43:57.378-07:00","display_name":"Abdelmajid Ainane","url":"https://independent.academia.edu/AbdelmajidAinane"},"attachments":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902607"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902607/A_Theoretical_Study_of_Hysteresis_Behaviors_of_2D_Mixed_Spin_1_2_1_Ising_Nanopaticles"><img alt="Research paper thumbnail of A Theoretical Study of Hysteresis Behaviors of 2D Mixed Spin-(1/2,1)Ising Nanopaticles" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902607/A_Theoretical_Study_of_Hysteresis_Behaviors_of_2D_Mixed_Spin_1_2_1_Ising_Nanopaticles">A Theoretical Study of Hysteresis Behaviors of 2D Mixed Spin-(1/2,1)Ising Nanopaticles</a></div><div class="wp-workCard_item"><span>2018 6th International Renewable and Sustainable Energy Conference (IRSEC)</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The EffectiveField Theory with correlations (EFT) based on the probability distribution is used t...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The EffectiveField Theory with correlations (EFT) based on the probability distribution is used to investigate the magnetic hysteresis behaviors of both hexagonal and square 2D nanoparticles consisting of a ferromagnetic spin-1/2 core and a ferromagnetic spin-l shell. The system parameters such as the ferrimagnetic exchange core/shell interaction, the surface shell exchange coupling and the reduced temperatureare examined on the magnetic hysteresis behaviors. Some interesting results have been found such as multiple hysteresis loop behaviors.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902607"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902607"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902607; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=72902607]").text(description); $(".js-view-count[data-work-id=72902607]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 72902607; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='72902607']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span></div><div id="work-strip-premium-row-container"></div></div></div><script> require.config({ waitSeconds: 90 })(["https://a.academia-assets.com/assets/wow_profile-a9bf3a2bc8c89fa2a77156577594264ee8a0f214d74241bc0fcd3f69f8d107ac.js","https://a.academia-assets.com/assets/work_edit-ad038b8c047c1a8d4fa01b402d530ff93c45fee2137a149a4a5398bc8ad67560.js"], function() { // from javascript_helper.rb var dispatcherData = {} if (false){ window.WowProfile.dispatcher = window.WowProfile.dispatcher || _.clone(Backbone.Events); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "-1" } } $('.js-work-strip[data-work-id=72902607]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":72902607,"title":"A Theoretical Study of Hysteresis Behaviors of 2D Mixed Spin-(1/2,1)Ising Nanopaticles","internal_url":"https://www.academia.edu/72902607/A_Theoretical_Study_of_Hysteresis_Behaviors_of_2D_Mixed_Spin_1_2_1_Ising_Nanopaticles","owner_id":14512644,"coauthors_can_edit":true,"owner":{"id":14512644,"first_name":"Abdelmajid","middle_initials":null,"last_name":"Ainane","page_name":"AbdelmajidAinane","domain_name":"independent","created_at":"2014-07-30T06:43:57.378-07:00","display_name":"Abdelmajid Ainane","url":"https://independent.academia.edu/AbdelmajidAinane"},"attachments":[]}, dispatcherData: dispatcherData }); $(this).data('initialized', true); } }); $a.trackClickSource(".js-work-strip-work-link", "profile_work_strip") }); </script> <div class="js-work-strip profile--work_container" data-work-id="72902601"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902601/Rational_Design_of_2D_h_BAs_Monolayer_as_Advanced_Sulfur_Host_for_High_Energy_Density_Li_S_Batteries"><img alt="Research paper thumbnail of Rational Design of 2D h-BAs Monolayer as Advanced Sulfur Host for High Energy Density Li–S Batteries" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902601/Rational_Design_of_2D_h_BAs_Monolayer_as_Advanced_Sulfur_Host_for_High_Energy_Density_Li_S_Batteries">Rational Design of 2D h-BAs Monolayer as Advanced Sulfur Host for High Energy Density Li–S Batteries</a></div><div class="wp-workCard_item"><span>ACS Applied Energy Materials</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The emergence of compact lithium-sulfur (Li-S) batteries with improved performances is becoming o...</span><a class="js-work-more-abstract" data-broccoli-component="work_strip.more_abstract" data-click-track="profile-work-strip-more-abstract" href="javascript:;"><span> more </span><span><i class="fa fa-caret-down"></i></span></a><span class="js-work-more-abstract-untruncated hidden">The emergence of compact lithium-sulfur (Li-S) batteries with improved performances is becoming one of the most desirable aspects of future energy technologies. Beyond Li-ion batteries, Li-S is of great relevance to follow as it adapts to the specificity of each application. It is among the most suitable elements for high-performance energy storage systems, given its high theoretical capacity (1674 mA h g(-1)) and energy density (2600 W h kg(-1)) relative to Li-ion batteries (300 W h kg(-1)). Nevertheless, the high-cell polarization and the shuttle effect constitute an enormous challenge toward the concrete applications of Li-S batteries. In the framework of this work, density functional theory calculations have been carried out to analyze the potential of h-BAs nanosheets as a promising host material for Li-S batteries. Binding and electronic characteristics of lithium polysulfides (LiPSs) adsorbed on h-BAs surface have been explored. Reported findings highlight the potential of the hBAs monolayer as a moderate host material, given that the binding energies of different LiPSs vary from 0.47 to 3.55 eV. More detailed analysis of the complex binding mechanisms is carried out by investigating the components of van der Waals physical/chemical interactions. The defected surface of the h-BAs monolayer has optimum binding energies with LiPSs for Li-S batteries. All these findings provide valuable insights into the binding and electronic characteristics of the h-BAs monolayer as a moderate host material for Li-S batteries.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902601"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902601"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902601; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); 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</script> <div class="js-work-strip profile--work_container" data-work-id="72902598"><div class="profile--work_thumbnail hidden-xs"><a class="js-work-strip-work-link" data-click-track="profile-work-strip-thumbnail" rel="nofollow" href="https://www.academia.edu/72902598/Electronic_optical_and_thermoelectric_properties_of_two_dimensional_pentagonal_SiGeC4_nanosheet_for_photovoltaic_applications_First_principles_calculations"><img alt="Research paper thumbnail of Electronic, optical and thermoelectric properties of two-dimensional pentagonal SiGeC4 nanosheet for photovoltaic applications: First-principles calculations" class="work-thumbnail" src="https://a.academia-assets.com/images/blank-paper.jpg" /></a></div><div class="wp-workCard wp-workCard_itemContainer"><div class="wp-workCard_item wp-workCard--title"><a class="js-work-strip-work-link text-gray-darker" data-click-track="profile-work-strip-title" rel="nofollow" href="https://www.academia.edu/72902598/Electronic_optical_and_thermoelectric_properties_of_two_dimensional_pentagonal_SiGeC4_nanosheet_for_photovoltaic_applications_First_principles_calculations">Electronic, optical and thermoelectric properties of two-dimensional pentagonal SiGeC4 nanosheet for photovoltaic applications: First-principles calculations</a></div><div class="wp-workCard_item"><span>Superlattices and Microstructures</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><span class="wp-workCard--action visible-if-viewed-by-owner inline-block" style="display: none;"><span class="js-profile-work-strip-edit-button-wrapper profile-work-strip-edit-button-wrapper" data-work-id="72902598"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="72902598"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 72902598; 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