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data-click-track="profile-expand-user-info-coauthors"><p class="label">Co-authors</p><p class="data">13</p></div></a><a href="/VBindilatti/mentions"><div class="stat-container"><p class="label">Mentions</p><p class="data">1</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="13233541" href="https://www.academia.edu/Documents/in/Space_and_Time_Philosophy_"><div id="js-react-on-rails-context" style="display:none" 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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 Valdir Bindilatti</h3></div><div class="js-work-strip profile--work_container" data-work-id="102966194"><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/102966194/System_for_critical_current_measurements_on_NbTi_superconducting_wires"><img alt="Research paper thumbnail of System for critical current measurements on NbTi superconducting wires" 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" href="https://www.academia.edu/102966194/System_for_critical_current_measurements_on_NbTi_superconducting_wires">System for critical current measurements on NbTi superconducting wires</a></div><div class="wp-workCard_item"><span>Revista de Fisica Aplicada e Instrumentacao</span><span>, 1989</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="102966194"><a class="js-profile-work-strip-edit-button" tabindex="0"><span><i class="fa 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Bindilatti","url":"https://independent.academia.edu/VBindilatti"},"attachments":[],"research_interests":[],"urls":[{"id":26616220,"url":"https://repositorio.usp.br/item/000760211"}]}, 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="85293010"><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/85293010/Magnetization_steps_due_to_pairs_of_distant_neighbor_spins_in_Zn1_xCoxSe_and_Zn1_xCoxS"><img alt="Research paper thumbnail of Magnetization steps due to pairs of distant-neighbor spins in Zn1-xCoxSe and Zn1-xCoxS" 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" href="https://www.academia.edu/85293010/Magnetization_steps_due_to_pairs_of_distant_neighbor_spins_in_Zn1_xCoxSe_and_Zn1_xCoxS">Magnetization steps due to pairs of distant-neighbor spins in Zn1-xCoxSe and Zn1-xCoxS</a></div><div class="wp-workCard_item"><span>Solid State Communications</span><span>, 1990</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">ABSTRACT Magnetization steps (MSTs) were observed in Zn1-xCoxSe and Zn1-xCoxS using temperatures ...</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">ABSTRACT Magnetization steps (MSTs) were observed in Zn1-xCoxSe and Zn1-xCoxS using temperatures T &amp;lt; 1 K, steady magnetic fields up to 200 kOe, and pulsed fields up to ∼400 kOe. Unlike the MSTs observed earlier in other materials, these MSTs are due to pairs of distant-neighbor spins rather than to pairs of nearest-neighbor spins. For Zn1-xCoxSe the results give a second-neighbor exchange constant J2/kB = −3.04±0.1 K, and suggest a third-neighbor exchange constant . An exchange constant J/kB = −2.25±0.2 K observed in Zn1-xCoxS is either J2 or J3.</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="85293010"><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="85293010"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 85293010; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=85293010]").text(description); $(".js-view-count[data-work-id=85293010]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 85293010; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='85293010']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 85293010, 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" } } $('.js-work-strip[data-work-id=85293010]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":85293010,"title":"Magnetization steps due to pairs of distant-neighbor spins in Zn1-xCoxSe and Zn1-xCoxS","translated_title":"","metadata":{"abstract":"ABSTRACT Magnetization steps (MSTs) were observed in Zn1-xCoxSe and Zn1-xCoxS using temperatures T \u0026amp;lt; 1 K, steady magnetic fields up to 200 kOe, and pulsed fields up to ∼400 kOe. Unlike the MSTs observed earlier in other materials, these MSTs are due to pairs of distant-neighbor spins rather than to pairs of nearest-neighbor spins. For Zn1-xCoxSe the results give a second-neighbor exchange constant J2/kB = −3.04±0.1 K, and suggest a third-neighbor exchange constant . An exchange constant J/kB = −2.25±0.2 K observed in Zn1-xCoxS is either J2 or J3.","publisher":"Elsevier BV","publication_date":{"day":null,"month":null,"year":1990,"errors":{}},"publication_name":"Solid State Communications"},"translated_abstract":"ABSTRACT Magnetization steps (MSTs) were observed in Zn1-xCoxSe and Zn1-xCoxS using temperatures T \u0026amp;lt; 1 K, steady magnetic fields up to 200 kOe, and pulsed fields up to ∼400 kOe. Unlike the MSTs observed earlier in other materials, these MSTs are due to pairs of distant-neighbor spins rather than to pairs of nearest-neighbor spins. For Zn1-xCoxSe the results give a second-neighbor exchange constant J2/kB = −3.04±0.1 K, and suggest a third-neighbor exchange constant . An exchange constant J/kB = −2.25±0.2 K observed in Zn1-xCoxS is either J2 or J3.","internal_url":"https://www.academia.edu/85293010/Magnetization_steps_due_to_pairs_of_distant_neighbor_spins_in_Zn1_xCoxSe_and_Zn1_xCoxS","translated_internal_url":"","created_at":"2022-08-21T11:24:25.515-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":13233541,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Magnetization_steps_due_to_pairs_of_distant_neighbor_spins_in_Zn1_xCoxSe_and_Zn1_xCoxS","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":13233541,"first_name":"Valdir","middle_initials":null,"last_name":"Bindilatti","page_name":"VBindilatti","domain_name":"independent","created_at":"2014-06-24T00:06:39.989-07:00","display_name":"Valdir Bindilatti","url":"https://independent.academia.edu/VBindilatti"},"attachments":[],"research_interests":[{"id":56,"name":"Materials Engineering","url":"https://www.academia.edu/Documents/in/Materials_Engineering"},{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics"},{"id":523,"name":"Chemistry","url":"https://www.academia.edu/Documents/in/Chemistry"},{"id":519549,"name":"Magnetization","url":"https://www.academia.edu/Documents/in/Magnetization"}],"urls":[]}, 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="76696922"><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/76696922/Exchange_bond_structure_and_magnetization_step_spectra_of_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Lopsided_two_exchange_models"><img alt="Research paper thumbnail of Exchange-bond structure and magnetization-step spectra of a diluted Heisenberg antiferromagnet on the square lattice: Lopsided two-exchange models" class="work-thumbnail" src="https://attachments.academia-assets.com/84943681/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/76696922/Exchange_bond_structure_and_magnetization_step_spectra_of_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Lopsided_two_exchange_models">Exchange-bond structure and magnetization-step spectra of a diluted Heisenberg antiferromagnet on the square lattice: Lopsided two-exchange models</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Theoretycal results on the magnetization and susceptibility of a Heisenberg diluted antiferromagn...</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">Theoretycal results on the magnetization and susceptibility of a Heisenberg diluted antiferromagnet in the square lattice are given. The models considered have two exchange constants (J1-J2 and J1-J3) of which the second is much smaller than the first (lopsided models). Cluster statistics for clusters with up to 5 spins is given. A procedure to account for the contribution to the magnetization of clusters with more than 5 spins is described.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="883eb73561977e701cecff2148967ed1" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":84943681,"asset_id":76696922,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/84943681/download_file?st=MTczMjc5MDgyNyw4LjIyMi4yMDguMTQ2&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="76696922"><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="76696922"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 76696922; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76696922]").text(description); $(".js-view-count[data-work-id=76696922]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76696922; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='76696922']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 76696922, 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: "883eb73561977e701cecff2148967ed1" } } $('.js-work-strip[data-work-id=76696922]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":76696922,"title":"Exchange-bond structure and magnetization-step spectra of a diluted Heisenberg antiferromagnet on the square lattice: Lopsided two-exchange models","translated_title":"","metadata":{"abstract":"Theoretycal results on the magnetization and susceptibility of a Heisenberg diluted antiferromagnet in the square lattice are given. 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A procedure to account for the contribution to the magnetization of clusters with more than 5 spins is described.","internal_url":"https://www.academia.edu/76696922/Exchange_bond_structure_and_magnetization_step_spectra_of_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Lopsided_two_exchange_models","translated_internal_url":"","created_at":"2022-04-17T04:24:10.283-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":13233541,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":84943681,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/84943681/thumbnails/1.jpg","file_name":"0609715.pdf","download_url":"https://www.academia.edu/attachments/84943681/download_file?st=MTczMjc5MDgyNyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Exchange_bond_structure_and_magnetizatio.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/84943681/0609715-libre.pdf?1650953360=\u0026response-content-disposition=attachment%3B+filename%3DExchange_bond_structure_and_magnetizatio.pdf\u0026Expires=1732794427\u0026Signature=Fzuj23QHCq4PUc6saneFIuIHg4kyvm6ZCQ4TfYfDNWdDMYdoIbjeDFR1ObJERUpDwSPoRQVzoiV~PMWPVUm6oJ-SHDyS7viFKdr-XpPQXevcIi-LCdT0oPCkpWuyxvv9TYQy1YxWEUc5N4xdi773TYlRidH0SbuwsKSQPvxL8Q6SJZkyF3SiIyCIZlCWmB7shcS0RBrBqPAt01QML1XTpZ73zjlxgSnA79-FILIIA8YFdC-cXFaa8ueZrDzLkcMOjgw4KZ94kD6uH~iMPCp8ytETY-Q9H3TMLO9eMB5ZXXWEX2f0FKfqcyHYiN1EPI2OdMMJkLAJSZdB-ix8bzELGQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Exchange_bond_structure_and_magnetization_step_spectra_of_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Lopsided_two_exchange_models","translated_slug":"","page_count":18,"language":"en","content_type":"Work","owner":{"id":13233541,"first_name":"Valdir","middle_initials":null,"last_name":"Bindilatti","page_name":"VBindilatti","domain_name":"independent","created_at":"2014-06-24T00:06:39.989-07:00","display_name":"Valdir Bindilatti","url":"https://independent.academia.edu/VBindilatti"},"attachments":[{"id":84943681,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/84943681/thumbnails/1.jpg","file_name":"0609715.pdf","download_url":"https://www.academia.edu/attachments/84943681/download_file?st=MTczMjc5MDgyNyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Exchange_bond_structure_and_magnetizatio.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/84943681/0609715-libre.pdf?1650953360=\u0026response-content-disposition=attachment%3B+filename%3DExchange_bond_structure_and_magnetizatio.pdf\u0026Expires=1732794427\u0026Signature=Fzuj23QHCq4PUc6saneFIuIHg4kyvm6ZCQ4TfYfDNWdDMYdoIbjeDFR1ObJERUpDwSPoRQVzoiV~PMWPVUm6oJ-SHDyS7viFKdr-XpPQXevcIi-LCdT0oPCkpWuyxvv9TYQy1YxWEUc5N4xdi773TYlRidH0SbuwsKSQPvxL8Q6SJZkyF3SiIyCIZlCWmB7shcS0RBrBqPAt01QML1XTpZ73zjlxgSnA79-FILIIA8YFdC-cXFaa8ueZrDzLkcMOjgw4KZ94kD6uH~iMPCp8ytETY-Q9H3TMLO9eMB5ZXXWEX2f0FKfqcyHYiN1EPI2OdMMJkLAJSZdB-ix8bzELGQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics"},{"id":520,"name":"Statistical Mechanics","url":"https://www.academia.edu/Documents/in/Statistical_Mechanics"},{"id":1220891,"name":"Antiferromagnetism","url":"https://www.academia.edu/Documents/in/Antiferromagnetism"}],"urls":[]}, 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="76696921"><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/76696921/Magnetization_steps_and_cluster_type_statistics_for_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Models_with_two_exchange_constants"><img alt="Research paper thumbnail of Magnetization steps and cluster-type statistics for a diluted Heisenberg antiferromagnet on the square lattice: Models with two exchange constants" class="work-thumbnail" src="https://attachments.academia-assets.com/84943781/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/76696921/Magnetization_steps_and_cluster_type_statistics_for_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Models_with_two_exchange_constants">Magnetization steps and cluster-type statistics for a diluted Heisenberg antiferromagnet on the square lattice: Models with two exchange constants</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The paper presents theoretical results on the magnetization of a diluted Heisenberg antiferromagn...</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 paper presents theoretical results on the magnetization of a diluted Heisenberg antiferromagnet on the square lattice for models with two exchange constants (J1-J2 and J1-J3). Cluster with up to five spins (5/2) are considered.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="9e4580d304b558a5bc78944ee9785544" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":84943781,"asset_id":76696921,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/84943781/download_file?st=MTczMjc5MDgyNyw4LjIyMi4yMDguMTQ2&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="76696921"><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="76696921"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 76696921; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76696921]").text(description); $(".js-view-count[data-work-id=76696921]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76696921; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='76696921']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 76696921, 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: "9e4580d304b558a5bc78944ee9785544" } } $('.js-work-strip[data-work-id=76696921]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":76696921,"title":"Magnetization steps and cluster-type statistics for a diluted Heisenberg antiferromagnet on the square lattice: Models with two exchange constants","translated_title":"","metadata":{"abstract":"The paper presents theoretical results on the magnetization of a diluted Heisenberg antiferromagnet on the square lattice for models with two exchange constants (J1-J2 and J1-J3). 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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="76696868"><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/76696868/Mixed_state_odd_Hall_effect_in_YBa2Cu3O7_with_unidirectional_twins"><img alt="Research paper thumbnail of Mixed state odd Hall effect in YBa2Cu3O7?? with unidirectional twins" 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" href="https://www.academia.edu/76696868/Mixed_state_odd_Hall_effect_in_YBa2Cu3O7_with_unidirectional_twins">Mixed state odd Hall effect in YBa2Cu3O7?? with unidirectional twins</a></div><div class="wp-workCard_item"><span>Journal of Low Temperature Physics</span><span>, 1996</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We have studied the mixed state Hall effect in YBa2Cu3O7−δ single crystals with unidirectional tw...</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 have studied the mixed state Hall effect in YBa2Cu3O7−δ single crystals with unidirectional twins: ϱxy=f(H). An analysis of the Hall conductivity σxy in free flux flow regime reveals that σxy can be successfully described by two terms which are related to the quasiparticle excitations and the motion of free vortices respectively. We have discovered the strong twin dependence of the Hall conductivity σxy in the pinning (TAFF) regime and detected the sign reverse of the Hall conductivity σxy at changing angle α (+45 °→−45 °) between current and twin plane that indicated the presence of backflow of vortices. We have observed that σxy tends to -∞ while approaching the melting line. These results provide the evidence of strong planar pinning influence on the Hall conductivity.</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="76696868"><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="76696868"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 76696868; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76696868]").text(description); $(".js-view-count[data-work-id=76696868]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76696868; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='76696868']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 76696868, 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" } } $('.js-work-strip[data-work-id=76696868]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":76696868,"title":"Mixed state odd Hall effect in YBa2Cu3O7?? with unidirectional twins","translated_title":"","metadata":{"abstract":"We have studied the mixed state Hall effect in YBa2Cu3O7−δ single crystals with unidirectional twins: ϱxy=f(H). An analysis of the Hall conductivity σxy in free flux flow regime reveals that σxy can be successfully described by two terms which are related to the quasiparticle excitations and the motion of free vortices respectively. We have discovered the strong twin dependence of the Hall conductivity σxy in the pinning (TAFF) regime and detected the sign reverse of the Hall conductivity σxy at changing angle α (+45 °→−45 °) between current and twin plane that indicated the presence of backflow of vortices. We have observed that σxy tends to -∞ while approaching the melting line. These results provide the evidence of strong planar pinning influence on the Hall conductivity.","publisher":"Springer Nature","publication_date":{"day":null,"month":null,"year":1996,"errors":{}},"publication_name":"Journal of Low Temperature Physics"},"translated_abstract":"We have studied the mixed state Hall effect in YBa2Cu3O7−δ single crystals with unidirectional twins: ϱxy=f(H). An analysis of the Hall conductivity σxy in free flux flow regime reveals that σxy can be successfully described by two terms which are related to the quasiparticle excitations and the motion of free vortices respectively. We have discovered the strong twin dependence of the Hall conductivity σxy in the pinning (TAFF) regime and detected the sign reverse of the Hall conductivity σxy at changing angle α (+45 °→−45 °) between current and twin plane that indicated the presence of backflow of vortices. We have observed that σxy tends to -∞ while approaching the melting line. These results provide the evidence of strong planar pinning influence on the Hall conductivity.","internal_url":"https://www.academia.edu/76696868/Mixed_state_odd_Hall_effect_in_YBa2Cu3O7_with_unidirectional_twins","translated_internal_url":"","created_at":"2022-04-17T04:23:22.936-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":13233541,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Mixed_state_odd_Hall_effect_in_YBa2Cu3O7_with_unidirectional_twins","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":13233541,"first_name":"Valdir","middle_initials":null,"last_name":"Bindilatti","page_name":"VBindilatti","domain_name":"independent","created_at":"2014-06-24T00:06:39.989-07:00","display_name":"Valdir Bindilatti","url":"https://independent.academia.edu/VBindilatti"},"attachments":[],"research_interests":[{"id":318,"name":"Mathematical 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class="work-thumbnail" src="https://attachments.academia-assets.com/71983083/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/56753766/Spin_glass_behavior_in_MnIn2Se4_and_Zn1_xMnxIn2Se4_magnetic_semiconductors">Spin glass behavior in MnIn2Se4 and Zn1−xMnxIn2Se4 magnetic semiconductors</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://independent.academia.edu/mantillajohn">john mantilla</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/VBindilatti">Valdir Bindilatti</a></span></div><div class="wp-workCard_item"><span>Journal of Magnetism and Magnetic Materials</span><span>, 2004</span></div><div class="wp-workCard_item 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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="55418707"><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/55418707/Evidence_for_the_Ising_Lifshitz_crossover_in_MnP"><img alt="Research paper thumbnail of Evidence for the Ising-Lifshitz crossover in MnP" 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" href="https://www.academia.edu/55418707/Evidence_for_the_Ising_Lifshitz_crossover_in_MnP">Evidence for the Ising-Lifshitz crossover in MnP</a></div><div class="wp-workCard_item"><span>Physical Review B</span><span>, 2000</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">ABSTRACT Manganese phosphide (MnP) is one of the few magnetic systems in which a uniaxial Lifshit...</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">ABSTRACT Manganese phosphide (MnP) is one of the few magnetic systems in which a uniaxial Lifshitz point (LP) has been identified. For the external magnetic field applied along the crystallographic b axis, the LP occurs at TL=121±1K and Hb=16.4kOe, at the confluence of modulated, ferromagnetic (F), and paramagnetic (P) phases. It has been shown that the magnetic susceptibility at fixed temperature (χ) as a function of Hb diverges at the F-P phase boundary with the specific heat exponent α. In this work χ×Hb was measured across the F-P phase boundary from T≈200K down to T=121K. From the analysis of the divergence, α was evaluated at different temperatures. For T well above TL, α≈0.12, a value close to the prediction for the three-dimensional Ising model. As T is lowered, the divergence gets sharper and α increases, reaching α=0.44 at TL, in agreement with predictions for this uniaxial LP.</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="55418707"><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="55418707"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 55418707; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=55418707]").text(description); $(".js-view-count[data-work-id=55418707]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 55418707; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='55418707']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 55418707, 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" } } $('.js-work-strip[data-work-id=55418707]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":55418707,"title":"Evidence for the Ising-Lifshitz crossover in MnP","translated_title":"","metadata":{"abstract":"ABSTRACT Manganese phosphide (MnP) is one of the few magnetic systems in which a uniaxial Lifshitz point (LP) has been identified. 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For T well above TL, α≈0.12, a value close to the prediction for the three-dimensional Ising model. 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Cluster with up to five spins (5/2) are considered.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="6d945cedd0ba5e577947eb9723446eaa" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46703577,"asset_id":26404433,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46703577/download_file?st=MTczMjc5MDgyOCw4LjIyMi4yMDguMTQ2&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="26404433"><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="26404433"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26404433; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=26404433]").text(description); $(".js-view-count[data-work-id=26404433]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 26404433; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='26404433']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 26404433, 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: "6d945cedd0ba5e577947eb9723446eaa" } } $('.js-work-strip[data-work-id=26404433]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":26404433,"title":"Magnetization steps and cluster-type statistics for a diluted Heisenberg antiferromagnet on the square lattice: Models with two exchange constants","translated_title":"","metadata":{"abstract":"The paper presents theoretical results on the magnetization of a diluted Heisenberg antiferromagnet on the square lattice for models with two exchange constants (J1-J2 and J1-J3). 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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="26404431"><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/26404431/Magnetization_step_spectra_of_CH3_NH3_2MnxCd1_xCl4_at_20_mK_Fine_structure_and_the_second_largest_exchange_constant"><img alt="Research paper thumbnail of Magnetization-step spectra of (CH3-NH3)2MnxCd1- xCl4 at 20 mK : Fine structure and the second-largest exchange constant" 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" href="https://www.academia.edu/26404431/Magnetization_step_spectra_of_CH3_NH3_2MnxCd1_xCl4_at_20_mK_Fine_structure_and_the_second_largest_exchange_constant">Magnetization-step spectra of (CH3-NH3)2MnxCd1- xCl4 at 20 mK : Fine structure and the second-largest exchange constant</a></div><div class="wp-workCard_item"><span>Physical Review B Condensed Matter and Materials Physics</span><span>, 2007</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The compounds (CH3-NH3)2MnxCd1-xCl4 are among the better physical realizations of a diluted Heise...</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 compounds (CH3-NH3)2MnxCd1-xCl4 are among the better physical realizations of a diluted Heisenberg antiferromagnet on the square lattice. The magnetization of three powder samples, with x=0.063 , 0.067, and 0.157, was measured at temperatures T≅20mK in magnetic fields B up to 17T . Magnetization-step (MST) spectra were obtained with a much higher resolution than in the earlier MST study at</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="26404431"><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="26404431"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26404431; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=26404431]").text(description); $(".js-view-count[data-work-id=26404431]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 26404431; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='26404431']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 26404431, 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" } } $('.js-work-strip[data-work-id=26404431]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":26404431,"title":"Magnetization-step spectra of (CH3-NH3)2MnxCd1- xCl4 at 20 mK : Fine structure and the second-largest exchange constant","translated_title":"","metadata":{"abstract":"The compounds (CH3-NH3)2MnxCd1-xCl4 are among the better physical realizations of a diluted Heisenberg antiferromagnet on the square lattice. 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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="85293010"><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/85293010/Magnetization_steps_due_to_pairs_of_distant_neighbor_spins_in_Zn1_xCoxSe_and_Zn1_xCoxS"><img alt="Research paper thumbnail of Magnetization steps due to pairs of distant-neighbor spins in Zn1-xCoxSe and Zn1-xCoxS" 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" href="https://www.academia.edu/85293010/Magnetization_steps_due_to_pairs_of_distant_neighbor_spins_in_Zn1_xCoxSe_and_Zn1_xCoxS">Magnetization steps due to pairs of distant-neighbor spins in Zn1-xCoxSe and Zn1-xCoxS</a></div><div class="wp-workCard_item"><span>Solid State Communications</span><span>, 1990</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">ABSTRACT Magnetization steps (MSTs) were observed in Zn1-xCoxSe and Zn1-xCoxS using temperatures ...</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">ABSTRACT Magnetization steps (MSTs) were observed in Zn1-xCoxSe and Zn1-xCoxS using temperatures T &amp;lt; 1 K, steady magnetic fields up to 200 kOe, and pulsed fields up to ∼400 kOe. Unlike the MSTs observed earlier in other materials, these MSTs are due to pairs of distant-neighbor spins rather than to pairs of nearest-neighbor spins. For Zn1-xCoxSe the results give a second-neighbor exchange constant J2/kB = −3.04±0.1 K, and suggest a third-neighbor exchange constant . An exchange constant J/kB = −2.25±0.2 K observed in Zn1-xCoxS is either J2 or J3.</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="85293010"><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="85293010"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 85293010; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=85293010]").text(description); $(".js-view-count[data-work-id=85293010]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 85293010; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='85293010']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 85293010, 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" } } $('.js-work-strip[data-work-id=85293010]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":85293010,"title":"Magnetization steps due to pairs of distant-neighbor spins in Zn1-xCoxSe and Zn1-xCoxS","translated_title":"","metadata":{"abstract":"ABSTRACT Magnetization steps (MSTs) were observed in Zn1-xCoxSe and Zn1-xCoxS using temperatures T \u0026amp;lt; 1 K, steady magnetic fields up to 200 kOe, and pulsed fields up to ∼400 kOe. Unlike the MSTs observed earlier in other materials, these MSTs are due to pairs of distant-neighbor spins rather than to pairs of nearest-neighbor spins. For Zn1-xCoxSe the results give a second-neighbor exchange constant J2/kB = −3.04±0.1 K, and suggest a third-neighbor exchange constant . An exchange constant J/kB = −2.25±0.2 K observed in Zn1-xCoxS is either J2 or J3.","publisher":"Elsevier BV","publication_date":{"day":null,"month":null,"year":1990,"errors":{}},"publication_name":"Solid State Communications"},"translated_abstract":"ABSTRACT Magnetization steps (MSTs) were observed in Zn1-xCoxSe and Zn1-xCoxS using temperatures T \u0026amp;lt; 1 K, steady magnetic fields up to 200 kOe, and pulsed fields up to ∼400 kOe. Unlike the MSTs observed earlier in other materials, these MSTs are due to pairs of distant-neighbor spins rather than to pairs of nearest-neighbor spins. For Zn1-xCoxSe the results give a second-neighbor exchange constant J2/kB = −3.04±0.1 K, and suggest a third-neighbor exchange constant . An exchange constant J/kB = −2.25±0.2 K observed in Zn1-xCoxS is either J2 or J3.","internal_url":"https://www.academia.edu/85293010/Magnetization_steps_due_to_pairs_of_distant_neighbor_spins_in_Zn1_xCoxSe_and_Zn1_xCoxS","translated_internal_url":"","created_at":"2022-08-21T11:24:25.515-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":13233541,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Magnetization_steps_due_to_pairs_of_distant_neighbor_spins_in_Zn1_xCoxSe_and_Zn1_xCoxS","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":13233541,"first_name":"Valdir","middle_initials":null,"last_name":"Bindilatti","page_name":"VBindilatti","domain_name":"independent","created_at":"2014-06-24T00:06:39.989-07:00","display_name":"Valdir Bindilatti","url":"https://independent.academia.edu/VBindilatti"},"attachments":[],"research_interests":[{"id":56,"name":"Materials Engineering","url":"https://www.academia.edu/Documents/in/Materials_Engineering"},{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics"},{"id":523,"name":"Chemistry","url":"https://www.academia.edu/Documents/in/Chemistry"},{"id":519549,"name":"Magnetization","url":"https://www.academia.edu/Documents/in/Magnetization"}],"urls":[]}, 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="76696922"><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/76696922/Exchange_bond_structure_and_magnetization_step_spectra_of_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Lopsided_two_exchange_models"><img alt="Research paper thumbnail of Exchange-bond structure and magnetization-step spectra of a diluted Heisenberg antiferromagnet on the square lattice: Lopsided two-exchange models" class="work-thumbnail" src="https://attachments.academia-assets.com/84943681/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/76696922/Exchange_bond_structure_and_magnetization_step_spectra_of_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Lopsided_two_exchange_models">Exchange-bond structure and magnetization-step spectra of a diluted Heisenberg antiferromagnet on the square lattice: Lopsided two-exchange models</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">Theoretycal results on the magnetization and susceptibility of a Heisenberg diluted antiferromagn...</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">Theoretycal results on the magnetization and susceptibility of a Heisenberg diluted antiferromagnet in the square lattice are given. The models considered have two exchange constants (J1-J2 and J1-J3) of which the second is much smaller than the first (lopsided models). Cluster statistics for clusters with up to 5 spins is given. A procedure to account for the contribution to the magnetization of clusters with more than 5 spins is described.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="883eb73561977e701cecff2148967ed1" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":84943681,"asset_id":76696922,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/84943681/download_file?st=MTczMjc5MDgyOCw4LjIyMi4yMDguMTQ2&st=MTczMjc5MDgyNyw4LjIyMi4yMDguMTQ2&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="76696922"><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="76696922"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 76696922; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76696922]").text(description); $(".js-view-count[data-work-id=76696922]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76696922; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='76696922']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 76696922, 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: "883eb73561977e701cecff2148967ed1" } } $('.js-work-strip[data-work-id=76696922]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":76696922,"title":"Exchange-bond structure and magnetization-step spectra of a diluted Heisenberg antiferromagnet on the square lattice: Lopsided two-exchange models","translated_title":"","metadata":{"abstract":"Theoretycal results on the magnetization and susceptibility of a Heisenberg diluted antiferromagnet in the square lattice are given. 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A procedure to account for the contribution to the magnetization of clusters with more than 5 spins is described.","internal_url":"https://www.academia.edu/76696922/Exchange_bond_structure_and_magnetization_step_spectra_of_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Lopsided_two_exchange_models","translated_internal_url":"","created_at":"2022-04-17T04:24:10.283-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":13233541,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":84943681,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/84943681/thumbnails/1.jpg","file_name":"0609715.pdf","download_url":"https://www.academia.edu/attachments/84943681/download_file?st=MTczMjc5MDgyOCw4LjIyMi4yMDguMTQ2&st=MTczMjc5MDgyNyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Exchange_bond_structure_and_magnetizatio.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/84943681/0609715-libre.pdf?1650953360=\u0026response-content-disposition=attachment%3B+filename%3DExchange_bond_structure_and_magnetizatio.pdf\u0026Expires=1732794427\u0026Signature=Fzuj23QHCq4PUc6saneFIuIHg4kyvm6ZCQ4TfYfDNWdDMYdoIbjeDFR1ObJERUpDwSPoRQVzoiV~PMWPVUm6oJ-SHDyS7viFKdr-XpPQXevcIi-LCdT0oPCkpWuyxvv9TYQy1YxWEUc5N4xdi773TYlRidH0SbuwsKSQPvxL8Q6SJZkyF3SiIyCIZlCWmB7shcS0RBrBqPAt01QML1XTpZ73zjlxgSnA79-FILIIA8YFdC-cXFaa8ueZrDzLkcMOjgw4KZ94kD6uH~iMPCp8ytETY-Q9H3TMLO9eMB5ZXXWEX2f0FKfqcyHYiN1EPI2OdMMJkLAJSZdB-ix8bzELGQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Exchange_bond_structure_and_magnetization_step_spectra_of_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Lopsided_two_exchange_models","translated_slug":"","page_count":18,"language":"en","content_type":"Work","owner":{"id":13233541,"first_name":"Valdir","middle_initials":null,"last_name":"Bindilatti","page_name":"VBindilatti","domain_name":"independent","created_at":"2014-06-24T00:06:39.989-07:00","display_name":"Valdir Bindilatti","url":"https://independent.academia.edu/VBindilatti"},"attachments":[{"id":84943681,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/84943681/thumbnails/1.jpg","file_name":"0609715.pdf","download_url":"https://www.academia.edu/attachments/84943681/download_file?st=MTczMjc5MDgyOCw4LjIyMi4yMDguMTQ2&st=MTczMjc5MDgyNyw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Exchange_bond_structure_and_magnetizatio.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/84943681/0609715-libre.pdf?1650953360=\u0026response-content-disposition=attachment%3B+filename%3DExchange_bond_structure_and_magnetizatio.pdf\u0026Expires=1732794427\u0026Signature=Fzuj23QHCq4PUc6saneFIuIHg4kyvm6ZCQ4TfYfDNWdDMYdoIbjeDFR1ObJERUpDwSPoRQVzoiV~PMWPVUm6oJ-SHDyS7viFKdr-XpPQXevcIi-LCdT0oPCkpWuyxvv9TYQy1YxWEUc5N4xdi773TYlRidH0SbuwsKSQPvxL8Q6SJZkyF3SiIyCIZlCWmB7shcS0RBrBqPAt01QML1XTpZ73zjlxgSnA79-FILIIA8YFdC-cXFaa8ueZrDzLkcMOjgw4KZ94kD6uH~iMPCp8ytETY-Q9H3TMLO9eMB5ZXXWEX2f0FKfqcyHYiN1EPI2OdMMJkLAJSZdB-ix8bzELGQ__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics"},{"id":520,"name":"Statistical Mechanics","url":"https://www.academia.edu/Documents/in/Statistical_Mechanics"},{"id":1220891,"name":"Antiferromagnetism","url":"https://www.academia.edu/Documents/in/Antiferromagnetism"}],"urls":[]}, 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="76696921"><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/76696921/Magnetization_steps_and_cluster_type_statistics_for_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Models_with_two_exchange_constants"><img alt="Research paper thumbnail of Magnetization steps and cluster-type statistics for a diluted Heisenberg antiferromagnet on the square lattice: Models with two exchange constants" class="work-thumbnail" src="https://attachments.academia-assets.com/84943781/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/76696921/Magnetization_steps_and_cluster_type_statistics_for_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Models_with_two_exchange_constants">Magnetization steps and cluster-type statistics for a diluted Heisenberg antiferromagnet on the square lattice: Models with two exchange constants</a></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">The paper presents theoretical results on the magnetization of a diluted Heisenberg antiferromagn...</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 paper presents theoretical results on the magnetization of a diluted Heisenberg antiferromagnet on the square lattice for models with two exchange constants (J1-J2 and J1-J3). Cluster with up to five spins (5/2) are considered.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="9e4580d304b558a5bc78944ee9785544" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":84943781,"asset_id":76696921,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/84943781/download_file?st=MTczMjc5MDgyOCw4LjIyMi4yMDguMTQ2&st=MTczMjc5MDgyNyw4LjIyMi4yMDguMTQ2&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="76696921"><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="76696921"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 76696921; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76696921]").text(description); $(".js-view-count[data-work-id=76696921]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76696921; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='76696921']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 76696921, 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: "9e4580d304b558a5bc78944ee9785544" } } $('.js-work-strip[data-work-id=76696921]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":76696921,"title":"Magnetization steps and cluster-type statistics for a diluted Heisenberg antiferromagnet on the square lattice: Models with two exchange constants","translated_title":"","metadata":{"abstract":"The paper presents theoretical results on the magnetization of a diluted Heisenberg antiferromagnet on the square lattice for models with two exchange constants (J1-J2 and J1-J3). 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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="76696868"><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/76696868/Mixed_state_odd_Hall_effect_in_YBa2Cu3O7_with_unidirectional_twins"><img alt="Research paper thumbnail of Mixed state odd Hall effect in YBa2Cu3O7?? with unidirectional twins" 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" href="https://www.academia.edu/76696868/Mixed_state_odd_Hall_effect_in_YBa2Cu3O7_with_unidirectional_twins">Mixed state odd Hall effect in YBa2Cu3O7?? with unidirectional twins</a></div><div class="wp-workCard_item"><span>Journal of Low Temperature Physics</span><span>, 1996</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">We have studied the mixed state Hall effect in YBa2Cu3O7−δ single crystals with unidirectional tw...</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 have studied the mixed state Hall effect in YBa2Cu3O7−δ single crystals with unidirectional twins: ϱxy=f(H). An analysis of the Hall conductivity σxy in free flux flow regime reveals that σxy can be successfully described by two terms which are related to the quasiparticle excitations and the motion of free vortices respectively. We have discovered the strong twin dependence of the Hall conductivity σxy in the pinning (TAFF) regime and detected the sign reverse of the Hall conductivity σxy at changing angle α (+45 °→−45 °) between current and twin plane that indicated the presence of backflow of vortices. We have observed that σxy tends to -∞ while approaching the melting line. These results provide the evidence of strong planar pinning influence on the Hall conductivity.</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="76696868"><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="76696868"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 76696868; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=76696868]").text(description); $(".js-view-count[data-work-id=76696868]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 76696868; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='76696868']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 76696868, 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" } } $('.js-work-strip[data-work-id=76696868]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":76696868,"title":"Mixed state odd Hall effect in YBa2Cu3O7?? with unidirectional twins","translated_title":"","metadata":{"abstract":"We have studied the mixed state Hall effect in YBa2Cu3O7−δ single crystals with unidirectional twins: ϱxy=f(H). An analysis of the Hall conductivity σxy in free flux flow regime reveals that σxy can be successfully described by two terms which are related to the quasiparticle excitations and the motion of free vortices respectively. We have discovered the strong twin dependence of the Hall conductivity σxy in the pinning (TAFF) regime and detected the sign reverse of the Hall conductivity σxy at changing angle α (+45 °→−45 °) between current and twin plane that indicated the presence of backflow of vortices. We have observed that σxy tends to -∞ while approaching the melting line. These results provide the evidence of strong planar pinning influence on the Hall conductivity.","publisher":"Springer Nature","publication_date":{"day":null,"month":null,"year":1996,"errors":{}},"publication_name":"Journal of Low Temperature Physics"},"translated_abstract":"We have studied the mixed state Hall effect in YBa2Cu3O7−δ single crystals with unidirectional twins: ϱxy=f(H). An analysis of the Hall conductivity σxy in free flux flow regime reveals that σxy can be successfully described by two terms which are related to the quasiparticle excitations and the motion of free vortices respectively. We have discovered the strong twin dependence of the Hall conductivity σxy in the pinning (TAFF) regime and detected the sign reverse of the Hall conductivity σxy at changing angle α (+45 °→−45 °) between current and twin plane that indicated the presence of backflow of vortices. We have observed that σxy tends to -∞ while approaching the melting line. These results provide the evidence of strong planar pinning influence on the Hall conductivity.","internal_url":"https://www.academia.edu/76696868/Mixed_state_odd_Hall_effect_in_YBa2Cu3O7_with_unidirectional_twins","translated_internal_url":"","created_at":"2022-04-17T04:23:22.936-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":13233541,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Mixed_state_odd_Hall_effect_in_YBa2Cu3O7_with_unidirectional_twins","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":13233541,"first_name":"Valdir","middle_initials":null,"last_name":"Bindilatti","page_name":"VBindilatti","domain_name":"independent","created_at":"2014-06-24T00:06:39.989-07:00","display_name":"Valdir Bindilatti","url":"https://independent.academia.edu/VBindilatti"},"attachments":[],"research_interests":[{"id":318,"name":"Mathematical Physics","url":"https://www.academia.edu/Documents/in/Mathematical_Physics"},{"id":498,"name":"Physics","url":"https://www.academia.edu/Documents/in/Physics"},{"id":505,"name":"Condensed Matter Physics","url":"https://www.academia.edu/Documents/in/Condensed_Matter_Physics"},{"id":71115,"name":"Low Temperature Physics","url":"https://www.academia.edu/Documents/in/Low_Temperature_Physics"}],"urls":[]}, 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="56753766"><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/56753766/Spin_glass_behavior_in_MnIn2Se4_and_Zn1_xMnxIn2Se4_magnetic_semiconductors"><img alt="Research paper thumbnail of Spin glass behavior in MnIn2Se4 and Zn1−xMnxIn2Se4 magnetic semiconductors" class="work-thumbnail" src="https://attachments.academia-assets.com/71983083/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/56753766/Spin_glass_behavior_in_MnIn2Se4_and_Zn1_xMnxIn2Se4_magnetic_semiconductors">Spin glass behavior in MnIn2Se4 and Zn1−xMnxIn2Se4 magnetic semiconductors</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://independent.academia.edu/mantillajohn">john mantilla</a> and <a class="" data-click-track="profile-work-strip-authors" href="https://independent.academia.edu/VBindilatti">Valdir Bindilatti</a></span></div><div class="wp-workCard_item"><span>Journal of Magnetism and Magnetic Materials</span><span>, 2004</span></div><div class="wp-workCard_item 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{"id":56753766,"title":"Spin glass behavior in MnIn2Se4 and Zn1−xMnxIn2Se4 magnetic semiconductors","translated_title":"","metadata":{"publisher":"Elsevier BV","grobid_abstract":"We present measurements of the magnetic and structural properties of the magnetic semiconductor MnIn 2 Se 4 and Zn 1Àx Mn x In 2 Se 4 ðx ¼ 0:87Þ: The localized Mn ions in the layered rhombohedral structure undergo a spin-freezing transition below 3:5 K: The frequency-dependent freezing temperature T f varies as DT f =ðT f D log oÞE0:022; indicating spin-glass behavior.","publication_date":{"day":null,"month":null,"year":2004,"errors":{}},"publication_name":"Journal of Magnetism and Magnetic 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{"id":55418827,"title":"Espectroscopia de interações de exchange por degraus de magnetização em semicondutores magnéticos diluidos","translated_title":"","metadata":{"publisher":"Universidade de Sao Paulo Sistema Integrado de Bibliotecas - 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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="55418707"><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/55418707/Evidence_for_the_Ising_Lifshitz_crossover_in_MnP"><img alt="Research paper thumbnail of Evidence for the Ising-Lifshitz crossover in MnP" 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" href="https://www.academia.edu/55418707/Evidence_for_the_Ising_Lifshitz_crossover_in_MnP">Evidence for the Ising-Lifshitz crossover in MnP</a></div><div class="wp-workCard_item"><span>Physical Review B</span><span>, 2000</span></div><div class="wp-workCard_item"><span class="js-work-more-abstract-truncated">ABSTRACT Manganese phosphide (MnP) is one of the few magnetic systems in which a uniaxial Lifshit...</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">ABSTRACT Manganese phosphide (MnP) is one of the few magnetic systems in which a uniaxial Lifshitz point (LP) has been identified. For the external magnetic field applied along the crystallographic b axis, the LP occurs at TL=121±1K and Hb=16.4kOe, at the confluence of modulated, ferromagnetic (F), and paramagnetic (P) phases. It has been shown that the magnetic susceptibility at fixed temperature (χ) as a function of Hb diverges at the F-P phase boundary with the specific heat exponent α. In this work χ×Hb was measured across the F-P phase boundary from T≈200K down to T=121K. From the analysis of the divergence, α was evaluated at different temperatures. For T well above TL, α≈0.12, a value close to the prediction for the three-dimensional Ising model. As T is lowered, the divergence gets sharper and α increases, reaching α=0.44 at TL, in agreement with predictions for this uniaxial LP.</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="55418707"><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="55418707"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 55418707; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=55418707]").text(description); $(".js-view-count[data-work-id=55418707]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 55418707; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='55418707']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 55418707, 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" } } $('.js-work-strip[data-work-id=55418707]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":55418707,"title":"Evidence for the Ising-Lifshitz crossover in MnP","translated_title":"","metadata":{"abstract":"ABSTRACT Manganese phosphide (MnP) is one of the few magnetic systems in which a uniaxial Lifshitz point (LP) has been identified. For the external magnetic field applied along the crystallographic b axis, the LP occurs at TL=121±1K and Hb=16.4kOe, at the confluence of modulated, ferromagnetic (F), and paramagnetic (P) phases. It has been shown that the magnetic susceptibility at fixed temperature (χ) as a function of Hb diverges at the F-P phase boundary with the specific heat exponent α. In this work χ×Hb was measured across the F-P phase boundary from T≈200K down to T=121K. From the analysis of the divergence, α was evaluated at different temperatures. For T well above TL, α≈0.12, a value close to the prediction for the three-dimensional Ising model. As T is lowered, the divergence gets sharper and α increases, reaching α=0.44 at TL, in agreement with predictions for this uniaxial LP.","publisher":"American Physical Society (APS)","publication_date":{"day":null,"month":null,"year":2000,"errors":{}},"publication_name":"Physical Review B"},"translated_abstract":"ABSTRACT Manganese phosphide (MnP) is one of the few magnetic systems in which a uniaxial Lifshitz point (LP) has been identified. For the external magnetic field applied along the crystallographic b axis, the LP occurs at TL=121±1K and Hb=16.4kOe, at the confluence of modulated, ferromagnetic (F), and paramagnetic (P) phases. It has been shown that the magnetic susceptibility at fixed temperature (χ) as a function of Hb diverges at the F-P phase boundary with the specific heat exponent α. In this work χ×Hb was measured across the F-P phase boundary from T≈200K down to T=121K. From the analysis of the divergence, α was evaluated at different temperatures. For T well above TL, α≈0.12, a value close to the prediction for the three-dimensional Ising model. As T is lowered, the divergence gets sharper and α increases, reaching α=0.44 at TL, in agreement with predictions for this uniaxial LP.","internal_url":"https://www.academia.edu/55418707/Evidence_for_the_Ising_Lifshitz_crossover_in_MnP","translated_internal_url":"","created_at":"2021-10-04T05:41:11.072-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":13233541,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[],"slug":"Evidence_for_the_Ising_Lifshitz_crossover_in_MnP","translated_slug":"","page_count":null,"language":"en","content_type":"Work","owner":{"id":13233541,"first_name":"Valdir","middle_initials":null,"last_name":"Bindilatti","page_name":"VBindilatti","domain_name":"independent","created_at":"2014-06-24T00:06:39.989-07:00","display_name":"Valdir Bindilatti","url":"https://independent.academia.edu/VBindilatti"},"attachments":[],"research_interests":[{"id":7715,"name":"Magnetic Materials","url":"https://www.academia.edu/Documents/in/Magnetic_Materials"},{"id":34754,"name":"Magnetic field","url":"https://www.academia.edu/Documents/in/Magnetic_field"},{"id":114618,"name":"Ising Model","url":"https://www.academia.edu/Documents/in/Ising_Model"},{"id":149117,"name":"Magnetic Susceptibility","url":"https://www.academia.edu/Documents/in/Magnetic_Susceptibility"},{"id":504035,"name":"Three Dimensional","url":"https://www.academia.edu/Documents/in/Three_Dimensional"},{"id":827572,"name":"Specific Heat","url":"https://www.academia.edu/Documents/in/Specific_Heat"},{"id":1130298,"name":"Critical Point","url":"https://www.academia.edu/Documents/in/Critical_Point"}],"urls":[]}, dispatcherData: dispatcherData }); 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Cluster with up to five spins (5/2) are considered.</span></div><div class="wp-workCard_item wp-workCard--actions"><span class="work-strip-bookmark-button-container"></span><a id="6d945cedd0ba5e577947eb9723446eaa" class="wp-workCard--action" rel="nofollow" data-click-track="profile-work-strip-download" data-download="{"attachment_id":46703577,"asset_id":26404433,"asset_type":"Work","button_location":"profile"}" href="https://www.academia.edu/attachments/46703577/download_file?st=MTczMjc5MDgyOCw4LjIyMi4yMDguMTQ2&st=MTczMjc5MDgyOCw4LjIyMi4yMDguMTQ2&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="26404433"><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="26404433"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26404433; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=26404433]").text(description); $(".js-view-count[data-work-id=26404433]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 26404433; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='26404433']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 26404433, 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: "6d945cedd0ba5e577947eb9723446eaa" } } $('.js-work-strip[data-work-id=26404433]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":26404433,"title":"Magnetization steps and cluster-type statistics for a diluted Heisenberg antiferromagnet on the square lattice: Models with two exchange constants","translated_title":"","metadata":{"abstract":"The paper presents theoretical results on the magnetization of a diluted Heisenberg antiferromagnet on the square lattice for models with two exchange constants (J1-J2 and J1-J3). 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Cluster with up to five spins (5/2) are considered.","internal_url":"https://www.academia.edu/26404433/Magnetization_steps_and_cluster_type_statistics_for_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Models_with_two_exchange_constants","translated_internal_url":"","created_at":"2016-06-22T04:36:56.445-07:00","preview_url":null,"current_user_can_edit":null,"current_user_is_owner":null,"owner_id":13233541,"coauthors_can_edit":true,"document_type":"paper","co_author_tags":[],"downloadable_attachments":[{"id":46703577,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/46703577/thumbnails/1.jpg","file_name":"Magnetization_steps_and_cluster-type_sta20160622-24434-17liabb.pdf","download_url":"https://www.academia.edu/attachments/46703577/download_file?st=MTczMjc5MDgyOCw4LjIyMi4yMDguMTQ2&st=MTczMjc5MDgyOCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Magnetization_steps_and_cluster_type_sta.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/46703577/Magnetization_steps_and_cluster-type_sta20160622-24434-17liabb-libre.pdf?1466595730=\u0026response-content-disposition=attachment%3B+filename%3DMagnetization_steps_and_cluster_type_sta.pdf\u0026Expires=1732794428\u0026Signature=JaGLSz34bBrI4xYUGyrVjZcsJU-hs3khZ4fB5CHyBOwIyDUu2Hp3lOCXLI4KD3TEQw5dk1ik~E45MzGhcPLXwjSgwxls~SZVi~LAfNmIWfhXceLxVO5xCDZXn4FFoDIfhYVCETeyv9hLVCcrlpDgZ8zhgbWk-cvsqhKfXJ40D46Zr1iGZ3AMKye32Y9GGRnijXWXpY36DwX0ifjhYT7KzDW-G2R8NUraZTe2tcPHmk7gZQ9Lj~hTJG~7LhcuWAuX-OrBeo8a3nqJ2qcCh-42eolGO-sG2~psJC937H8mlbCjr3fGUsFZhS1dzGhPWuZLSRol7aDnc4xnGG-dyXFg0w__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"slug":"Magnetization_steps_and_cluster_type_statistics_for_a_diluted_Heisenberg_antiferromagnet_on_the_square_lattice_Models_with_two_exchange_constants","translated_slug":"","page_count":16,"language":"en","content_type":"Work","owner":{"id":13233541,"first_name":"Valdir","middle_initials":null,"last_name":"Bindilatti","page_name":"VBindilatti","domain_name":"independent","created_at":"2014-06-24T00:06:39.989-07:00","display_name":"Valdir Bindilatti","url":"https://independent.academia.edu/VBindilatti"},"attachments":[{"id":46703577,"title":"","file_type":"pdf","scribd_thumbnail_url":"https://attachments.academia-assets.com/46703577/thumbnails/1.jpg","file_name":"Magnetization_steps_and_cluster-type_sta20160622-24434-17liabb.pdf","download_url":"https://www.academia.edu/attachments/46703577/download_file?st=MTczMjc5MDgyOCw4LjIyMi4yMDguMTQ2&st=MTczMjc5MDgyOCw4LjIyMi4yMDguMTQ2&","bulk_download_file_name":"Magnetization_steps_and_cluster_type_sta.pdf","bulk_download_url":"https://d1wqtxts1xzle7.cloudfront.net/46703577/Magnetization_steps_and_cluster-type_sta20160622-24434-17liabb-libre.pdf?1466595730=\u0026response-content-disposition=attachment%3B+filename%3DMagnetization_steps_and_cluster_type_sta.pdf\u0026Expires=1732794428\u0026Signature=JaGLSz34bBrI4xYUGyrVjZcsJU-hs3khZ4fB5CHyBOwIyDUu2Hp3lOCXLI4KD3TEQw5dk1ik~E45MzGhcPLXwjSgwxls~SZVi~LAfNmIWfhXceLxVO5xCDZXn4FFoDIfhYVCETeyv9hLVCcrlpDgZ8zhgbWk-cvsqhKfXJ40D46Zr1iGZ3AMKye32Y9GGRnijXWXpY36DwX0ifjhYT7KzDW-G2R8NUraZTe2tcPHmk7gZQ9Lj~hTJG~7LhcuWAuX-OrBeo8a3nqJ2qcCh-42eolGO-sG2~psJC937H8mlbCjr3fGUsFZhS1dzGhPWuZLSRol7aDnc4xnGG-dyXFg0w__\u0026Key-Pair-Id=APKAJLOHF5GGSLRBV4ZA"}],"research_interests":[{"id":520,"name":"Statistical Mechanics","url":"https://www.academia.edu/Documents/in/Statistical_Mechanics"},{"id":95016,"name":"Lattice Beam Model","url":"https://www.academia.edu/Documents/in/Lattice_Beam_Model"}],"urls":[{"id":7239018,"url":"http://adsabs.harvard.edu/abs/2006cond.mat..9701S"}]}, dispatcherData: dispatcherData }); 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The magnetization of three powder samples, with x=0.063 , 0.067, and 0.157, was measured at temperatures T≅20mK in magnetic fields B up to 17T . Magnetization-step (MST) spectra were obtained with a much higher resolution than in the earlier MST study at</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="26404431"><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="26404431"><i class="fa fa-spinner fa-spin"></i></span><script>$(function () { var workId = 26404431; window.Academia.workViewCountsFetcher.queue(workId, function (count) { var description = window.$h.commaizeInt(count) + " " + window.$h.pluralize(count, 'View'); $(".js-view-count[data-work-id=26404431]").text(description); $(".js-view-count[data-work-id=26404431]").attr('title', description).tooltip(); }); });</script></span></span><span><span class="percentile-widget hidden"><span class="u-mr2x work-percentile"></span></span><script>$(function () { var workId = 26404431; window.Academia.workPercentilesFetcher.queue(workId, function (percentileText) { var container = $(".js-work-strip[data-work-id='26404431']"); container.find('.work-percentile').text(percentileText.charAt(0).toUpperCase() + percentileText.slice(1)); container.find('.percentile-widget').show(); container.find('.percentile-widget').removeClass('hidden'); }); });</script></span><span><script>$(function() { new Works.PaperRankView({ workId: 26404431, 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" } } $('.js-work-strip[data-work-id=26404431]').each(function() { if (!$(this).data('initialized')) { new WowProfile.WorkStripView({ el: this, workJSON: {"id":26404431,"title":"Magnetization-step spectra of (CH3-NH3)2MnxCd1- xCl4 at 20 mK : Fine structure and the second-largest exchange constant","translated_title":"","metadata":{"abstract":"The compounds (CH3-NH3)2MnxCd1-xCl4 are among the better physical realizations of a diluted Heisenberg antiferromagnet on the square lattice. The magnetization of three powder samples, with x=0.063 , 0.067, and 0.157, was measured at temperatures T≅20mK in magnetic fields B up to 17T . Magnetization-step (MST) spectra were obtained with a much higher resolution than in the earlier MST study at","publication_date":{"day":null,"month":null,"year":2007,"errors":{}},"publication_name":"Physical Review B Condensed Matter and Materials Physics"},"translated_abstract":"The compounds (CH3-NH3)2MnxCd1-xCl4 are among the better physical realizations of a diluted Heisenberg antiferromagnet on the square lattice. The magnetization of three powder samples, with x=0.063 , 0.067, and 0.157, was measured at temperatures T≅20mK in magnetic fields B up to 17T . 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