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class="label">Followers</p><p class="data">10</p></div></a><a><div class="stat-container js-profile-followees" data-broccoli-component="user-info.followees-count" data-click-track="profile-expand-user-info-following"><p class="label">Following</p><p class="data">9</p></div></a><a><div class="stat-container js-profile-coauthors" data-broccoli-component="user-info.coauthors-count" data-click-track="profile-expand-user-info-coauthors"><p class="label">Co-authors</p><p class="data">8</p></div></a><span><div class="stat-container"><p class="label"><span class="js-profile-total-view-text">Public Views</span></p><p class="data"><span class="js-profile-view-count"></span></p></div></span></div><div class="ri-section"><div class="ri-section-header"><span>Interests</span></div><div class="ri-tags-container"><a data-click-track="profile-user-info-expand-research-interests" data-has-card-for-ri-list="32519121" href="https://www.academia.edu/Documents/in/Semiconductor_Nanostructures"><div 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data-dom-id="Pill-react-component-85c4e5e6-3c46-4510-9b45-961f92757951"></div> <div id="Pill-react-component-85c4e5e6-3c46-4510-9b45-961f92757951"></div> </a><a data-click-track="profile-user-info-expand-research-interests" data-has-card-for-ri-list="32519121" href="https://www.academia.edu/Documents/in/Dualism"><div class="js-react-on-rails-component" style="display:none" data-component-name="Pill" data-props="{"color":"gray","children":["Dualism"]}" data-trace="false" data-dom-id="Pill-react-component-ce67157d-83eb-4cc1-acc0-77332dedb9bf"></div> <div id="Pill-react-component-ce67157d-83eb-4cc1-acc0-77332dedb9bf"></div> </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 C. Batista</h3></div><div class="js-work-strip profile--work_container" data-work-id="13946707"><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/13946707/Quest_for_band_renormalization_and_self_energy_In_correlated_f_electron_systems"><img alt="Research paper thumbnail of Quest for band renormalization and self-energy In correlated f-electron systems" class="work-thumbnail" src="https://attachments.academia-assets.com/44777674/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/13946707/Quest_for_band_renormalization_and_self_energy_In_correlated_f_electron_systems">Quest for band renormalization and self-energy In correlated f-electron systems</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://uppsala.academia.edu/PeterOppeneer">Peter Oppeneer</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/CBatista1">C. Batista</a></span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="3b87c2bc96c567761d0b0f75dfdcdef0" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":44777674,"asset_id":13946707,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/44777674/download_file?st=MTczMjQ3Njc1OSw4LjIyMi4yMDguMTQ2&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="13946707"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="13946707"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 13946707; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=13946707]").text(description); $(".js-view-count[data-work-id=13946707]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 13946707; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='13946707']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 13946707, container: "", }); });</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-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.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); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "3b87c2bc96c567761d0b0f75dfdcdef0" } } $('.js-work-strip[data-work-id=13946707]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":13946707,"title":"Quest for band renormalization and self-energy In correlated f-electron systems","translated_title":"","metadata":{"grobid_abstract":"Coexisting low-energy scales are observed in f -electron materials. The information about some of low-energy scales is imprinted in the electron self-energy, which can be measured by angle-resolved photoemission (ARPES). Such measurements in d-electron materials over the last decade were based on high energy-and momentumresolution ARPES techniques used to extract the self-energy information from measured spectra. Simultaneously, many-body theoretical approaches have been developed to find a link between the self-energy and many-body interactions. Here we show the transcription of such methods from d-electrons to f -electrons by presenting the first example of low energy scales in the f -electron material USb2, measured with synchrotron-based ARPES. The proposed approach will help in answering the fundamental questions about the complex nature of the heavy fermion state.","publication_date":{"day":null,"month":null,"year":2010,"errors":{}},"grobid_abstract_attachment_id":44777674},"translated_abstract":null,"internal_url":"https://www.academia.edu/13946707/Quest_for_band_renormalization_and_self_energy_In_correlated_f_electron_systems","translated_internal_url":"","created_at":"2015-07-12T06:56:13.325-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":33002203,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":2938980,"work_id":13946707,"tagging_user_id":33002203,"tagged_user_id":234666035,"co_author_invite_id":753962,"email":"y***n@fudan.edu.cn","display_order":0,"name":"yinglin yang","title":"Quest for band renormalization and self-energy In correlated f-electron systems"},{"id":18488995,"work_id":13946707,"tagging_user_id":33002203,"tagged_user_id":33235407,"co_author_invite_id":null,"email":"p***r@temple.edu","display_order":4194304,"name":"P. 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Batista</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://cambridge.academia.edu/SiddharthmontuSaxena">Siddharth S Saxena</a></span></div><div class="wp-workCard_item"><span>Journal of Physics: Condensed Matter</span><span>, 2011</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="b6ff40a7d85e9dcf8b3ee9bee40985ff" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":42994474,"asset_id":22366954,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/42994474/download_file?st=MTczMjQ3Njc1OSw4LjIyMi4yMDguMTQ2&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="22366954"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="22366954"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 22366954; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=22366954]").text(description); $(".js-view-count[data-work-id=22366954]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 22366954; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='22366954']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 22366954, container: "", }); });</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-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.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); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "b6ff40a7d85e9dcf8b3ee9bee40985ff" } } $('.js-work-strip[data-work-id=22366954]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":22366954,"title":"Strongly correlated electron systems","translated_title":"","metadata":{"publication_date":{"day":null,"month":null,"year":2011,"errors":{}},"publication_name":"Journal of Physics: Condensed Matter"},"translated_abstract":null,"internal_url":"https://www.academia.edu/22366954/Strongly_correlated_electron_systems","translated_internal_url":"","created_at":"2016-02-23T16:57:25.280-08:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":27440,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":15966964,"work_id":22366954,"tagging_user_id":27440,"tagged_user_id":32519121,"co_author_invite_id":null,"email":"c***b@lanl.gov","display_order":0,"name":"C. 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alt="Research paper thumbnail of Crystal symmetry and high-magnetic-field specific heat of SrCU2(BO3)(2" class="work-thumbnail" src="https://attachments.academia-assets.com/49944721/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/4317588/Crystal_symmetry_and_high_magnetic_field_specific_heat_of_SrCU2_BO3_2">Crystal symmetry and high-magnetic-field specific heat of SrCU2(BO3)(2</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://kbfi.academia.edu/RaivoStern">Raivo Stern</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/CBatista1">C. Batista</a></span></div><div class="wp-workCard_item"><span>Physical Review B</span><span>, 2005</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="3164a8c038c57676c63cfcaadb9d7e39" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":49944721,"asset_id":4317588,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/49944721/download_file?st=MTczMjQ3Njc1OSw4LjIyMi4yMDguMTQ2&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="4317588"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="4317588"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 4317588; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=4317588]").text(description); $(".js-view-count[data-work-id=4317588]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 4317588; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='4317588']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 4317588, container: "", }); });</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-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.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); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "3164a8c038c57676c63cfcaadb9d7e39" } } $('.js-work-strip[data-work-id=4317588]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":4317588,"title":"Crystal symmetry and high-magnetic-field specific heat of SrCU2(BO3)(2","translated_title":"","metadata":{"grobid_abstract":"We report measurements of the specific heat of the quantum spin liquid system SrCu2(BO3)2 in continuous magnetic fields H of up to 33 T. 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The ground states of this model are exactly obtained at a first order quantum phase transition between two regions with different valence bond solid order parameters. At this point, the low energy excitations are deconfined spinons and spin-charge separation occurs under doping in the limit of low concentration of holes. In addition, this point is characterized by the proliferation of topological defects that signal the emergence of Z2 gauge symmetry. PACS numbers: 71.27.+a, 71.28.+d, Frustrated magnets are the focus of considerable attention because exotic quantum effects are expected to emerge from the competition between two or more opposite tendencies. While several models in this category are solvable in one dimension, the list is much smaller for higher dimensions. One of the most studied frustrated magnets is the spin 1/2 Heisenberg model with first and second nearest neighbor interactions J 1 and J 2 . In one dimension, this model exhibits a quantum transition as a function of J 2 /J 1 from a critical state with quasi-long range antiferromagnetic (AF) order to a dimerized phase. Moreover, the exact dimerized ground state has been obtained for the point J 2 /J 1 = 0.5 by Majumdar and Ghosh [1]. In contrast, two dimensional (2D) frustrated magnets like the J 1 − J 2 Heisenberg model on a square lattice still hold many secrets. Different approaches predict a transition between a Néel ordered state and a gapped (non-magnetic) quantum phase for the region 0.4 J 2 /J 1 0.6. However, the nature of this phase is still debated. More precisely, the question is whether it is a uniform spin liquid [2, 3] or a spatially ordered valence bond crystal .","publication_date":{"day":null,"month":null,"year":2004,"errors":{}},"publication_name":"Physical Review Letters","grobid_abstract_attachment_id":45540262},"translated_abstract":null,"internal_url":"https://www.academia.edu/13259789/Exact_Ground_States_of_a_Frustrated_2D_Magnet_Deconfined_Fractional_Excitations_at_a_First_Order_Quantum_Phase_Transition","translated_internal_url":"","created_at":"2015-06-24T22:40:51.507-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":32519121,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":1515055,"work_id":13259789,"tagging_user_id":32519121,"tagged_user_id":null,"co_author_invite_id":473897,"email":"s***t@lanl.gov","display_order":0,"name":"S. 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Batista</a>, <a class="" data-click-track="profile-work-strip-authors" href="https://uncu.academia.edu/AAAligia">A. Aligia</a>, and <a class="" data-click-track="profile-work-strip-authors" href="https://bdp.academia.edu/AlejandroMart%C3%ADnLobos">Alejandro Martín Lobos</a></span></div><div class="wp-workCard_item"><span>Physical Review B</span><span>, 2005</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="016398aea039d8e170b173fc349bf74b" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":45611812,"asset_id":13180551,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/45611812/download_file?st=MTczMjQ3Njc1OSw4LjIyMi4yMDguMTQ2&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="13180551"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="13180551"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 13180551; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=13180551]").text(description); $(".js-view-count[data-work-id=13180551]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 13180551; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='13180551']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 13180551, container: "", }); });</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-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.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); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "016398aea039d8e170b173fc349bf74b" } } $('.js-work-strip[data-work-id=13180551]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":13180551,"title":"Anisotropic intermediate valence in Yb2M3Ga9 (M=Rh,Ir)","translated_title":"","metadata":{"grobid_abstract":"The intermediate valence compounds Yb 2 M 3 Ga 9 (M = Rh, Ir) exhibit an anisotropic magnetic susceptibility. We report measurements of the temperature dependence of the 4f occupation number, n f (T), for Yb 2 M 3 Ga 9 as well as the magnetic inelastic neutron scattering spectrum S mag (∆E) at 12 and 300 K for Yb 2 Rh 3 Ga 9 . Both n f (T) and S mag (∆E) were calculated for the Anderson impurity model with crystal field terms within an approach based on the non-crossing approximation. 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Fisk</a>, <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/CBatista1">C. Batista</a>, <a class="" data-click-track="profile-work-strip-authors" href="https://uncu.academia.edu/AAAligia">A. Aligia</a>, and <a class="" data-click-track="profile-work-strip-authors" href="https://bdp.academia.edu/AlejandroMart%C3%ADnLobos">Alejandro Martín Lobos</a></span></div><div class="wp-workCard_item"><span>Physical Review B</span><span>, 2005</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="095359fe2d92219536f03e89ef343ea0" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":45611821,"asset_id":13180553,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/45611821/download_file?st=MTczMjQ3Njc1OSw4LjIyMi4yMDguMTQ2&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="13180553"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="13180553"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 13180553; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=13180553]").text(description); $(".js-view-count[data-work-id=13180553]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 13180553; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='13180553']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 13180553, container: "", }); });</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-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.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); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "095359fe2d92219536f03e89ef343ea0" } } $('.js-work-strip[data-work-id=13180553]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":13180553,"title":"Crystal-field effects in the mixed-valence compounds Yb2M3Ga9 (M=Rh,Ir)","translated_title":"","metadata":{"grobid_abstract":"Magnetic susceptibility, heat capacity, and electrical resistivity measurements have been carried out on single crystals of the intermediate valence compounds Yb2Rh3Ga9 and Yb2Ir3Ga9. 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The rhizome, rootlets, and root hairs produce medicinally active alkaloids. Berberine, one of the Hydrastis alkaloids, has shown antifungal activity. The influence of a combination of the major Hydrastis alkaloids on the plant rhizosphere fungal ecology has not been investigated. A bioassay was developed to study the effect of goldenseal isoquinoline alkaloids on three Fusarium isolates, including the two species isolated from Hydrastis rhizosphere. The findings suggest that the Hydrastis root extract influences macroconidia germination, but that only the combined alkaloids--berberine, canadine, and hydrastine--appear to synergistically stimulate production of the mycotoxin zearalenone in the Fusarium oxysporum isolate. The Hydrastis root rhizosphere effect provided a selective advantage to the Fusarium isolates closely associated with the root tissue in comparison with the Fusarium isolate that had never been exposed to Hydrastis.</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="13259786"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="13259786"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 13259786; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=13259786]").text(description); $(".js-view-count[data-work-id=13259786]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 13259786; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='13259786']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 13259786, container: "", }); });</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-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.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" } } $('.js-work-strip[data-work-id=13259786]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":13259786,"title":"Effects of Root Isoquinoline Alkaloids from Hydrastis canadensis on Fusarium oxysporum Isolated from Hydrastis Root Tissue","translated_title":"","metadata":{"abstract":"Goldenseal (Hydrastis canadensis L.) is a popular medicinal plant distributed widely in North America. 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The findings suggest that the Hydrastis root extract influences macroconidia germination, but that only the combined alkaloids--berberine, canadine, and hydrastine--appear to synergistically stimulate production of the mycotoxin zearalenone in the Fusarium oxysporum isolate. The Hydrastis root rhizosphere effect provided a selective advantage to the Fusarium isolates closely associated with the root tissue in comparison with the Fusarium isolate that had never been exposed to Hydrastis.","internal_url":"https://www.academia.edu/13259786/Effects_of_Root_Isoquinoline_Alkaloids_from_Hydrastis_canadensis_on_Fusarium_oxysporum_Isolated_from_Hydrastis_Root_Tissue","translated_internal_url":"","created_at":"2015-06-24T22:40:51.107-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":32519121,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":1515058,"work_id":13259786,"tagging_user_id":32519121,"tagged_user_id":null,"co_author_invite_id":473898,"email":"m***s@nist.gov","display_order":0,"name":"Michael Tims","title":"Effects of Root Isoquinoline Alkaloids from Hydrastis canadensis on Fusarium oxysporum Isolated from Hydrastis Root Tissue"}],"downloadable_attachments":[],"slug":"Effects_of_Root_Isoquinoline_Alkaloids_from_Hydrastis_canadensis_on_Fusarium_oxysporum_Isolated_from_Hydrastis_Root_Tissue","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":32519121,"first_name":"C.","middle_initials":null,"last_name":"Batista","page_name":"CBatista1","domain_name":"independent","created_at":"2015-06-24T22:40:23.647-07:00","display_name":"C. 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Batista</a>, and <a class="" data-click-track="profile-work-strip-authors" href="https://cnrs.academia.edu/MichelAvignon">Michel Avignon</a></span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We study numerically the one-dimensional ferromagnetic Kondo lattice model, which is widely used ...</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">We study numerically the one-dimensional ferromagnetic Kondo lattice model, which is widely used to describe nickel and manganese perovskites. We find broad regions near the commensurate dopings where the formation of magnetic polarons induces a charge-ordered state. This ordering arises from the competition between double and super-exchange, and is present even in the absence of any inter-site Coulomb repulsion. An</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="13201164"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="13201164"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 13201164; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=13201164]").text(description); $(".js-view-count[data-work-id=13201164]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 13201164; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='13201164']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 13201164, container: "", }); });</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-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.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" } } $('.js-work-strip[data-work-id=13201164]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":13201164,"title":"New Type or Charge and Magnetic Order in the Ferromagnetic Kondo Lattice","translated_title":"","metadata":{"abstract":"We study numerically the one-dimensional ferromagnetic Kondo lattice model, which is widely used to describe nickel and manganese perovskites. We find broad regions near the commensurate dopings where the formation of magnetic polarons induces a charge-ordered state. This ordering arises from the competition between double and super-exchange, and is present even in the absence of any inter-site Coulomb repulsion. An","publication_date":{"day":null,"month":null,"year":2001,"errors":{}}},"translated_abstract":"We study numerically the one-dimensional ferromagnetic Kondo lattice model, which is widely used to describe nickel and manganese perovskites. We find broad regions near the commensurate dopings where the formation of magnetic polarons induces a charge-ordered state. This ordering arises from the competition between double and super-exchange, and is present even in the absence of any inter-site Coulomb repulsion. An","internal_url":"https://www.academia.edu/13201164/New_Type_or_Charge_and_Magnetic_Order_in_the_Ferromagnetic_Kondo_Lattice","translated_internal_url":"","created_at":"2015-06-23T02:50:22.342-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":32457626,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":1402684,"work_id":13201164,"tagging_user_id":32457626,"tagged_user_id":52353215,"co_author_invite_id":446184,"email":"g***d@cab.cnea.gov.ar","display_order":-5033164,"name":"Daniel Garcia","title":"New Type or Charge and Magnetic Order in the Ferromagnetic Kondo Lattice"},{"id":1402687,"work_id":13201164,"tagging_user_id":32457626,"tagged_user_id":32519121,"co_author_invite_id":435347,"email":"c***b@lanl.gov","display_order":-1677721,"name":"C. 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Batista</a></span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="3b87c2bc96c567761d0b0f75dfdcdef0" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":44777674,"asset_id":13946707,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/44777674/download_file?st=MTczMjQ3Njc1OSw4LjIyMi4yMDguMTQ2&st=MTczMjQ3Njc1OSw4LjIyMi4yMDguMTQ2&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="13946707"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="13946707"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 13946707; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=13946707]").text(description); $(".js-view-count[data-work-id=13946707]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 13946707; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='13946707']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 13946707, container: "", }); });</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-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.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); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "3b87c2bc96c567761d0b0f75dfdcdef0" } } $('.js-work-strip[data-work-id=13946707]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":13946707,"title":"Quest for band renormalization and self-energy In correlated f-electron systems","translated_title":"","metadata":{"grobid_abstract":"Coexisting low-energy scales are observed in f -electron materials. The information about some of low-energy scales is imprinted in the electron self-energy, which can be measured by angle-resolved photoemission (ARPES). Such measurements in d-electron materials over the last decade were based on high energy-and momentumresolution ARPES techniques used to extract the self-energy information from measured spectra. Simultaneously, many-body theoretical approaches have been developed to find a link between the self-energy and many-body interactions. Here we show the transcription of such methods from d-electrons to f -electrons by presenting the first example of low energy scales in the f -electron material USb2, measured with synchrotron-based ARPES. The proposed approach will help in answering the fundamental questions about the complex nature of the heavy fermion state.","publication_date":{"day":null,"month":null,"year":2010,"errors":{}},"grobid_abstract_attachment_id":44777674},"translated_abstract":null,"internal_url":"https://www.academia.edu/13946707/Quest_for_band_renormalization_and_self_energy_In_correlated_f_electron_systems","translated_internal_url":"","created_at":"2015-07-12T06:56:13.325-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":33002203,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":2938980,"work_id":13946707,"tagging_user_id":33002203,"tagged_user_id":234666035,"co_author_invite_id":753962,"email":"y***n@fudan.edu.cn","display_order":0,"name":"yinglin yang","title":"Quest for band renormalization and self-energy In correlated f-electron systems"},{"id":18488995,"work_id":13946707,"tagging_user_id":33002203,"tagged_user_id":33235407,"co_author_invite_id":null,"email":"p***r@temple.edu","display_order":4194304,"name":"P. 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alt="Research paper thumbnail of Crystal symmetry and high-magnetic-field specific heat of SrCU2(BO3)(2" class="work-thumbnail" src="https://attachments.academia-assets.com/49944721/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/4317588/Crystal_symmetry_and_high_magnetic_field_specific_heat_of_SrCU2_BO3_2">Crystal symmetry and high-magnetic-field specific heat of SrCU2(BO3)(2</a></div><div class="wp-workCard_item wp-workCard--coauthors"><span>by </span><span><a class="" data-click-track="profile-work-strip-authors" href="https://kbfi.academia.edu/RaivoStern">Raivo Stern</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/CBatista1">C. Batista</a></span></div><div class="wp-workCard_item"><span>Physical Review B</span><span>, 2005</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="3164a8c038c57676c63cfcaadb9d7e39" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":49944721,"asset_id":4317588,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/49944721/download_file?st=MTczMjQ3Njc1OSw4LjIyMi4yMDguMTQ2&st=MTczMjQ3Njc1OSw4LjIyMi4yMDguMTQ2&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="4317588"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="4317588"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 4317588; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=4317588]").text(description); $(".js-view-count[data-work-id=4317588]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 4317588; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='4317588']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 4317588, container: "", }); });</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-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.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); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "3164a8c038c57676c63cfcaadb9d7e39" } } $('.js-work-strip[data-work-id=4317588]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":4317588,"title":"Crystal symmetry and high-magnetic-field specific heat of SrCU2(BO3)(2","translated_title":"","metadata":{"grobid_abstract":"We report measurements of the specific heat of the quantum spin liquid system SrCu2(BO3)2 in continuous magnetic fields H of up to 33 T. The specific heat data, when combined with a finite temperature Lanczos diagonalization of the Shastry-Sutherland Hamiltonian, indicates the presence of a nearest neighbor Dzyaloshinsky-Moriya (DM) interaction that violates the crystal symmetry for H = 0. Moreover, the same DM interaction is required to explain the observed ESR lines for H c. 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The ground states of this model are exactly obtained at a first order quantum phase transition between two regions with different valence bond solid order parameters. At this point, the low energy excitations are deconfined spinons and spin-charge separation occurs under doping in the limit of low concentration of holes. In addition, this point is characterized by the proliferation of topological defects that signal the emergence of Z2 gauge symmetry. PACS numbers: 71.27.+a, 71.28.+d, Frustrated magnets are the focus of considerable attention because exotic quantum effects are expected to emerge from the competition between two or more opposite tendencies. While several models in this category are solvable in one dimension, the list is much smaller for higher dimensions. One of the most studied frustrated magnets is the spin 1/2 Heisenberg model with first and second nearest neighbor interactions J 1 and J 2 . In one dimension, this model exhibits a quantum transition as a function of J 2 /J 1 from a critical state with quasi-long range antiferromagnetic (AF) order to a dimerized phase. Moreover, the exact dimerized ground state has been obtained for the point J 2 /J 1 = 0.5 by Majumdar and Ghosh [1]. In contrast, two dimensional (2D) frustrated magnets like the J 1 − J 2 Heisenberg model on a square lattice still hold many secrets. Different approaches predict a transition between a Néel ordered state and a gapped (non-magnetic) quantum phase for the region 0.4 J 2 /J 1 0.6. However, the nature of this phase is still debated. More precisely, the question is whether it is a uniform spin liquid [2, 3] or a spatially ordered valence bond crystal .","publication_date":{"day":null,"month":null,"year":2004,"errors":{}},"publication_name":"Physical Review Letters","grobid_abstract_attachment_id":45540262},"translated_abstract":null,"internal_url":"https://www.academia.edu/13259789/Exact_Ground_States_of_a_Frustrated_2D_Magnet_Deconfined_Fractional_Excitations_at_a_First_Order_Quantum_Phase_Transition","translated_internal_url":"","created_at":"2015-06-24T22:40:51.507-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":32519121,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":1515055,"work_id":13259789,"tagging_user_id":32519121,"tagged_user_id":null,"co_author_invite_id":473897,"email":"s***t@lanl.gov","display_order":0,"name":"S. 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Batista</a>, <a class="" data-click-track="profile-work-strip-authors" href="https://uncu.academia.edu/AAAligia">A. Aligia</a>, and <a class="" data-click-track="profile-work-strip-authors" href="https://bdp.academia.edu/AlejandroMart%C3%ADnLobos">Alejandro Martín Lobos</a></span></div><div class="wp-workCard_item"><span>Physical Review B</span><span>, 2005</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="016398aea039d8e170b173fc349bf74b" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":45611812,"asset_id":13180551,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/45611812/download_file?st=MTczMjQ3Njc1OSw4LjIyMi4yMDguMTQ2&st=MTczMjQ3Njc1OSw4LjIyMi4yMDguMTQ2&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="13180551"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="13180551"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 13180551; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=13180551]").text(description); $(".js-view-count[data-work-id=13180551]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 13180551; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='13180551']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 13180551, container: "", }); });</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-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.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); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "016398aea039d8e170b173fc349bf74b" } } $('.js-work-strip[data-work-id=13180551]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":13180551,"title":"Anisotropic intermediate valence in Yb2M3Ga9 (M=Rh,Ir)","translated_title":"","metadata":{"grobid_abstract":"The intermediate valence compounds Yb 2 M 3 Ga 9 (M = Rh, Ir) exhibit an anisotropic magnetic susceptibility. 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Fisk</a>, <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/CBatista1">C. Batista</a>, <a class="" data-click-track="profile-work-strip-authors" href="https://uncu.academia.edu/AAAligia">A. Aligia</a>, and <a class="" data-click-track="profile-work-strip-authors" href="https://bdp.academia.edu/AlejandroMart%C3%ADnLobos">Alejandro Martín Lobos</a></span></div><div class="wp-workCard_item"><span>Physical Review B</span><span>, 2005</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="095359fe2d92219536f03e89ef343ea0" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":45611821,"asset_id":13180553,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/45611821/download_file?st=MTczMjQ3Njc1OSw4LjIyMi4yMDguMTQ2&st=MTczMjQ3Njc1OSw4LjIyMi4yMDguMTQ2&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="13180553"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="13180553"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 13180553; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=13180553]").text(description); $(".js-view-count[data-work-id=13180553]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 13180553; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='13180553']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 13180553, container: "", }); });</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-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.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); dispatcherData = { dispatcher: window.WowProfile.dispatcher, downloadLinkId: "095359fe2d92219536f03e89ef343ea0" } } $('.js-work-strip[data-work-id=13180553]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":13180553,"title":"Crystal-field effects in the mixed-valence compounds Yb2M3Ga9 (M=Rh,Ir)","translated_title":"","metadata":{"grobid_abstract":"Magnetic susceptibility, heat capacity, and electrical resistivity measurements have been carried out on single crystals of the intermediate valence compounds Yb2Rh3Ga9 and Yb2Ir3Ga9. These measurements reveal a large anisotropy due apparently to an interplay between crystalline electric field (CEF) and Kondo effects. The temperature dependence of magnetic susceptibility can be modelled using the Anderson impurity model including CEF within an approach based on the Non-Crossing Approximation.","publication_date":{"day":null,"month":null,"year":2005,"errors":{}},"publication_name":"Physical Review B","grobid_abstract_attachment_id":45611821},"translated_abstract":null,"internal_url":"https://www.academia.edu/13180553/Crystal_field_effects_in_the_mixed_valence_compounds_Yb2M3Ga9_M_Rh_Ir_","translated_internal_url":"","created_at":"2015-06-22T11:27:44.711-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":32436904,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[{"id":1363890,"work_id":13180553,"tagging_user_id":32436904,"tagged_user_id":43204814,"co_author_invite_id":435348,"email":"z***k@ucdavis.edu","display_order":-5991862,"name":"Z. 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B <span xmlns:xlink="http://www.w3.org/1999/xlink" style="font-weight: bold;">75</span>, 094411 (2007)]</a></div><div class="wp-workCard_item"><span>Physical Review B</span><span>, 2013</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="13259788"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa fa-pencil"></i></span><span>Edit</span></a></span></span><span id="work-strip-rankings-button-container"></span></div><div class="wp-workCard_item wp-workCard--stats"><span><span><span class="js-view-count view-count u-mr2x" data-work-id="13259788"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 13259788; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=13259788]").text(description); $(".js-view-count[data-work-id=13259788]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 13259788; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='13259788']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 13259788, container: "", }); });</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-f77ea15d77ce96025a6048a514272ad8becbad23c641fc2b3bd6e24ca6ff1932.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" } } $('.js-work-strip[data-work-id=13259788]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":13259788,"title":"Erratum: High-dimensional fractionalization and spinon deconfinement in pyrochlore antiferromagnets [Phys. 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The rhizome, rootlets, and root hairs produce medicinally active alkaloids. Berberine, one of the Hydrastis alkaloids, has shown antifungal activity. The influence of a combination of the major Hydrastis alkaloids on the plant rhizosphere fungal ecology has not been investigated. A bioassay was developed to study the effect of goldenseal isoquinoline alkaloids on three Fusarium isolates, including the two species isolated from Hydrastis rhizosphere. The findings suggest that the Hydrastis root extract influences macroconidia germination, but that only the combined alkaloids--berberine, canadine, and hydrastine--appear to synergistically stimulate production of the mycotoxin zearalenone in the Fusarium oxysporum isolate. 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This ordering arises from the competition between double and super-exchange, and is present even in the absence of any inter-site Coulomb repulsion. 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