{"id":10411,"date":"2024-06-28T14:11:43","date_gmt":"2024-06-28T12:11:43","guid":{"rendered":"https:\/\/lncmi.cnrs.fr\/?page_id=9829"},"modified":"2025-07-07T10:42:09","modified_gmt":"2025-07-07T08:42:09","slug":"strongly-correlated-fermions","status":"publish","type":"page","link":"https:\/\/lncmi.cnrs.fr\/en\/highly-correlated-electronic-systems\/strongly-correlated-fermions\/","title":{"rendered":"Strongly correlated fermions"},"content":{"rendered":"<p>[et_pb_section fb_built=&#8221;1&#8243; fullwidth=&#8221;on&#8221; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_fullwidth_header title=&#8221;@ET-DC@eyJkeW5hbWljIjp0cnVlLCJjb250ZW50IjoicG9zdF90aXRsZSIsInNldHRpbmdzIjp7ImJlZm9yZSI6IiIsImFmdGVyIjoiIiwiZW5hYmxlX2h0bWwiOiJvZmYifX0=@&#8221; text_orientation=&#8221;center&#8221; background_overlay_color=&#8221;rgba(0,0,0,0.2)&#8221; _builder_version=&#8221;4.25.2&#8243; _dynamic_attributes=&#8221;title&#8221; _module_preset=&#8221;default&#8221; background_image=&#8221;https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2024\/07\/fond-style-abstract-fire_1017-3291.jpg&#8221; text_shadow_style=&#8221;preset3&#8243; global_colors_info=&#8221;{}&#8221;][\/et_pb_fullwidth_header][\/et_pb_section][et_pb_section fb_built=&#8221;1&#8243; disabled_on=&#8221;on|on|off&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; sticky_position=&#8221;top&#8221; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_row column_structure=&#8221;1_6,1_6,1_6,1_6,1_6,1_6&#8243; disabled_on=&#8221;off|off|off&#8221; _builder_version=&#8221;4.26.0&#8243; _module_preset=&#8221;default&#8221; sticky_position=&#8221;top&#8221; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;1_6&#8243; _builder_version=&#8221;4.26.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_button button_url=&#8221;#description&#8221; button_text=&#8221;Description&#8221; 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global_colors_info=&#8221;{}&#8221;][\/et_pb_button][\/et_pb_column][et_pb_column type=&#8221;1_6&#8243; _builder_version=&#8221;4.26.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_button button_url=&#8221;#themes&#8221; button_text=&#8221;Topics&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; custom_button=&#8221;on&#8221; button_text_size=&#8221;15px&#8221; global_colors_info=&#8221;{}&#8221;][\/et_pb_button][\/et_pb_column][et_pb_column type=&#8221;1_6&#8243; _builder_version=&#8221;4.26.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_button button_url=&#8221;#techniques&#8221; button_text=&#8221;Techniques&#8221; _builder_version=&#8221;4.26.0&#8243; _module_preset=&#8221;default&#8221; custom_button=&#8221;on&#8221; button_text_size=&#8221;15px&#8221; global_colors_info=&#8221;{}&#8221;][\/et_pb_button][\/et_pb_column][et_pb_column type=&#8221;1_6&#8243; _builder_version=&#8221;4.26.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_button button_url=&#8221;#publications&#8221; button_text=&#8221;Publications&#8221; _builder_version=&#8221;4.27.0&#8243; _module_preset=&#8221;default&#8221; custom_button=&#8221;on&#8221; button_text_size=&#8221;15px&#8221; global_colors_info=&#8221;{}&#8221;][\/et_pb_button][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=&#8221;1&#8243; admin_label=&#8221;Descriptions&#8221; module_id=&#8221;description&#8221; _builder_version=&#8221;4.27.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_row column_structure=&#8221;1_2,1_2&#8243; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;1_2&#8243; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_text _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<div class=\"prose prose-neutral max-w-none select-text overflow-x-auto text-wrap break-words dark:prose-invert prose-p:whitespace-break-spaces prose-code:m-0 prose-code:whitespace-break-spaces prose-pre:m-0 prose-pre:bg-[#1e1e1e] prose-pre:p-0 prose-ol:pl-8 font-light\">\n<p><strong>Strongly correlated fermions<\/strong> are elementary particles (like electrons) whose mutual interactions play a crucial role and cannot be neglected. The term is often used in the context of <strong>condensed matter physics<\/strong> to describe systems where the collective behavior of particles is highly complex and cannot be explained by simple free electron models.<\/p>\n<p>The study of strongly correlated fermions at LNCMI explores complex systems where particle interactions give rise to astonishing physical properties, often inaccessible without the use of intense magnetic fields<\/p>\n<p><span style=\"font-size: 14px\"><\/span><\/p>\n<p><span style=\"font-size: 14px\">Picture :<span class=\"wd-jnl-art-breadcrumb-title article-toolbar-anchor\"><span><a href=\"https:\/\/iopscience.iop.org\/journal\/0034-4885\" class=\"event_breadcrumb\" data-event-action=\"Title link\">Reports on Progress in Physics<\/a><\/span><\/span><span>,\u00a0<\/span><span class=\"wd-jnl-art-breadcrumb-vol nowrap\"><span><a href=\"https:\/\/iopscience.iop.org\/volume\/0034-4885\/79\" class=\"event_breadcrumb\" data-event-action=\"Volume link\">Volume 79<\/a><\/span><\/span><span>,\u00a0<\/span><span class=\"wd-jnl-art-breadcrumb-issue\"><a href=\"https:\/\/iopscience.iop.org\/issue\/0034-4885\/79\/9\" class=\"event_breadcrumb\" data-event-action=\"Issue link\">Number 9<\/a><\/span><\/span><span style=\"font-size: 14px\"><\/span><\/p>\n<\/div>\n<p>[\/et_pb_text][\/et_pb_column][et_pb_column type=&#8221;1_2&#8243; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_image src=&#8221;https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/02\/phase-diagram.jpg&#8221; title_text=&#8221;phase diagram&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; width=&#8221;56.1%&#8221; module_alignment=&#8221;center&#8221; custom_margin=&#8221;||19px|||&#8221; custom_padding=&#8221;|||0px||&#8221; global_colors_info=&#8221;{}&#8221;][\/et_pb_image][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=&#8221;1&#8243; admin_label=&#8221;Annuaire&#8221; module_id=&#8221;personnel&#8221; _builder_version=&#8221;4.27.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_row _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_text _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<h3>Research staff<\/h3>\n<p>[\/et_pb_text][et_pb_code _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<div class='rt-container-fluid rt-team-container rt-pos-r rt-team-container-10444' id='rt-team-container-2340044792'  data-layout='layout2' data-desktop-col='2'  data-tab-col='2'  data-mobile-col='1' data-sc-id='10444' data-popup-bg=''><div data-title='Loading ...' class='rt-row rt-content-loader layout2 ttp-even ttp-pre-loader'><div class=\"rt-col-md-6 rt-col-sm-6 rt-col-xs-12  even-grid-item rt-grid-item\" data-id=\"17762\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"17762\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/altangerel-munkhtuguldur\/\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"300\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2024\/12\/Munkhtuguldur_ALTANGEREL.jpg\" class=\"img-responsive rt-team-img\" alt=\"ALTANGEREL Munkhtuguldur\" \/><\/a><\/figure><\/div><div class=\"rttm-content-area rt-col-sm-10 rt-col-xs-8 \"><h3><span class=\"team-name\"><a class=\"\" data-id=\"17762\" target=\"_self\" title=\"ALTANGEREL Munkhtuguldur\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/altangerel-munkhtuguldur\/\">ALTANGEREL Munkhtuguldur<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"17762\" target=\"_self\" title=\"ALTANGEREL Munkhtuguldur\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/altangerel-munkhtuguldur\/\">PhD Student<\/a><\/div><div class=\"contact-info\"><ul><li class=\"tlp-location\"><i class=\"fa fa-map-marker\"><\/i><span class=\"tlp-location\">Toulouse<\/span><\/li><\/ul><\/div><\/div><\/div><\/div><div class=\"rt-col-md-6 rt-col-sm-6 rt-col-xs-12  even-grid-item rt-grid-item\" data-id=\"17631\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"17631\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/de-oliveira-rodrigues-gabriel\/\"><img loading=\"lazy\" decoding=\"async\" width=\"1536\" height=\"1536\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2024\/09\/picto-portrait-1536x1536.jpg\" class=\"img-responsive rt-team-img\" alt=\"DE OLIVEIRA RODRIGUES Gabriel\" \/><\/a><\/figure><\/div><div class=\"rttm-content-area rt-col-sm-10 rt-col-xs-8 \"><h3><span class=\"team-name\"><a class=\"\" data-id=\"17631\" target=\"_self\" title=\"DE OLIVEIRA RODRIGUES Gabriel\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/de-oliveira-rodrigues-gabriel\/\">DE OLIVEIRA RODRIGUES Gabriel<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"17631\" target=\"_self\" title=\"DE OLIVEIRA RODRIGUES Gabriel\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/de-oliveira-rodrigues-gabriel\/\">PhD Student<\/a><\/div><div class=\"contact-info\"><ul><li class=\"tlp-location\"><i class=\"fa fa-map-marker\"><\/i><span class=\"tlp-location\">Toulouse<\/span><\/li><\/ul><\/div><\/div><\/div><\/div><div class=\"rt-col-md-6 rt-col-sm-6 rt-col-xs-12  even-grid-item rt-grid-item\" data-id=\"17634\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"17634\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/duffy-caitlin\/\"><img loading=\"lazy\" decoding=\"async\" width=\"1536\" height=\"1536\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2024\/09\/picto-portrait-1536x1536.jpg\" class=\"img-responsive rt-team-img\" alt=\"DUFFY Caitlin\" \/><\/a><\/figure><\/div><div class=\"rttm-content-area rt-col-sm-10 rt-col-xs-8 \"><h3><span class=\"team-name\"><a class=\"\" data-id=\"17634\" target=\"_self\" title=\"DUFFY Caitlin\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/duffy-caitlin\/\">DUFFY Caitlin<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"17634\" target=\"_self\" title=\"DUFFY Caitlin\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/duffy-caitlin\/\">Postdoctoral Researcher<\/a><\/div><div class=\"contact-info\"><ul><li class=\"tlp-location\"><i class=\"fa fa-map-marker\"><\/i><span class=\"tlp-location\">Toulouse<\/span><\/li><\/ul><\/div><\/div><\/div><\/div><div class=\"rt-col-md-6 rt-col-sm-6 rt-col-xs-12  even-grid-item rt-grid-item\" data-id=\"25176\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"25176\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/le-mardele-florian-2\/\"><img loading=\"lazy\" decoding=\"async\" width=\"160\" height=\"160\" class=\"default-img\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/plugins\/tlp-team\/assets\/images\/demo.jpg\" alt=\"Default Image\" \/><\/a><\/figure><\/div><div class=\"rttm-content-area rt-col-sm-10 rt-col-xs-8 \"><h3><span class=\"team-name\"><a class=\"\" data-id=\"25176\" target=\"_self\" title=\"LE MARDELE Florian\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/le-mardele-florian-2\/\">LE MARDELE Florian<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"25176\" target=\"_self\" title=\"LE MARDELE Florian\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/le-mardele-florian-2\/\">Postdoctoral Researcher<\/a><\/div><div class=\"contact-info\"><ul><li class=\"tlp-location\"><i class=\"fa fa-map-marker\"><\/i><span class=\"tlp-location\">Toulouse<\/span><\/li><\/ul><\/div><\/div><\/div><\/div><div class=\"rt-col-md-6 rt-col-sm-6 rt-col-xs-12  even-grid-item rt-grid-item\" data-id=\"17718\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"17718\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/leboeuf-david\/\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"300\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/05\/David_LEBOEUF.jpg\" class=\"img-responsive rt-team-img\" alt=\"LEBOEUF David\" \/><\/a><\/figure><\/div><div class=\"rttm-content-area rt-col-sm-10 rt-col-xs-8 \"><h3><span class=\"team-name\"><a class=\"\" data-id=\"17718\" target=\"_self\" title=\"LEBOEUF David\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/leboeuf-david\/\">LEBOEUF David<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"17718\" target=\"_self\" title=\"LEBOEUF David\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/leboeuf-david\/\">Researcher<\/a><\/div><div class=\"contact-info\"><ul><li class=\"tlp-location\"><i class=\"fa fa-map-marker\"><\/i><span class=\"tlp-location\">Grenoble<\/span><\/li><\/ul><\/div><\/div><\/div><\/div><div class=\"rt-col-md-6 rt-col-sm-6 rt-col-xs-12  even-grid-item rt-grid-item\" data-id=\"17607\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"17607\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/marquardt-nils\/\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"300\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2024\/12\/Nils_MARQUARDT.jpg\" class=\"img-responsive rt-team-img\" alt=\"MARQUARDT Nils\" \/><\/a><\/figure><\/div><div class=\"rttm-content-area rt-col-sm-10 rt-col-xs-8 \"><h3><span class=\"team-name\"><a class=\"\" data-id=\"17607\" target=\"_self\" title=\"MARQUARDT Nils\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/marquardt-nils\/\">MARQUARDT Nils<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"17607\" target=\"_self\" title=\"MARQUARDT Nils\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/marquardt-nils\/\">PhD Student<\/a><\/div><div class=\"contact-info\"><ul><li class=\"tlp-location\"><i class=\"fa fa-map-marker\"><\/i><span class=\"tlp-location\">Grenoble<\/span><\/li><\/ul><\/div><\/div><\/div><\/div><div class=\"rt-col-md-6 rt-col-sm-6 rt-col-xs-12  even-grid-item rt-grid-item\" data-id=\"17734\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"17734\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/mayaffre-hadrien\/\"><img loading=\"lazy\" decoding=\"async\" width=\"400\" height=\"533\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2024\/07\/MAYAFFRE-400x533-1.jpg\" class=\"img-responsive rt-team-img\" alt=\"MAYAFFRE Hadrien\" \/><\/a><\/figure><\/div><div class=\"rttm-content-area rt-col-sm-10 rt-col-xs-8 \"><h3><span class=\"team-name\"><a class=\"\" data-id=\"17734\" target=\"_self\" title=\"MAYAFFRE Hadrien\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/mayaffre-hadrien\/\">MAYAFFRE Hadrien<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"17734\" target=\"_self\" title=\"MAYAFFRE Hadrien\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/mayaffre-hadrien\/\">Associate professor<\/a><\/div><div class=\"contact-info\"><ul><li class=\"tlp-location\"><i class=\"fa fa-map-marker\"><\/i><span class=\"tlp-location\">Grenoble<\/span><\/li><\/ul><\/div><\/div><\/div><\/div><div class=\"rt-col-md-6 rt-col-sm-6 rt-col-xs-12  even-grid-item rt-grid-item\" data-id=\"17722\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"17722\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/proust-cyril\/\"><img loading=\"lazy\" decoding=\"async\" width=\"227\" height=\"300\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2024\/09\/cyril2-227x300-1.jpg\" class=\"img-responsive rt-team-img\" alt=\"PROUST Cyril\" \/><\/a><\/figure><\/div><div class=\"rttm-content-area rt-col-sm-10 rt-col-xs-8 \"><h3><span class=\"team-name\"><a class=\"\" data-id=\"17722\" target=\"_self\" title=\"PROUST Cyril\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/proust-cyril\/\">PROUST Cyril<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"17722\" target=\"_self\" title=\"PROUST Cyril\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/proust-cyril\/\">Researcher<\/a><\/div><div class=\"contact-info\"><ul><li class=\"tlp-location\"><i class=\"fa fa-map-marker\"><\/i><span class=\"tlp-location\">Toulouse<\/span><\/li><\/ul><\/div><\/div><\/div><\/div><div class=\"rt-col-md-6 rt-col-sm-6 rt-col-xs-12  even-grid-item rt-grid-item\" data-id=\"24252\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"24252\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/schliebach-anne\/\"><img loading=\"lazy\" decoding=\"async\" width=\"160\" height=\"160\" class=\"default-img\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/plugins\/tlp-team\/assets\/images\/demo.jpg\" alt=\"Default Image\" \/><\/a><\/figure><\/div><div class=\"rttm-content-area rt-col-sm-10 rt-col-xs-8 \"><h3><span class=\"team-name\"><a class=\"\" data-id=\"24252\" target=\"_self\" title=\"SCHLIEBACH Anne\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/schliebach-anne\/\">SCHLIEBACH Anne<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"24252\" target=\"_self\" title=\"SCHLIEBACH Anne\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/schliebach-anne\/\">Doctorante<\/a><\/div><div class=\"contact-info\"><ul><li class=\"tlp-location\"><i class=\"fa fa-map-marker\"><\/i><span class=\"tlp-location\">Grenoble<\/span><\/li><\/ul><\/div><\/div><\/div><\/div><div class=\"rt-col-md-6 rt-col-sm-6 rt-col-xs-12  even-grid-item rt-grid-item\" data-id=\"17669\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"17669\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/schuchard-mathilde\/\"><img loading=\"lazy\" decoding=\"async\" width=\"1536\" height=\"1536\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2024\/09\/picto-portrait-1536x1536.jpg\" class=\"img-responsive rt-team-img\" alt=\"SCHUCHARD Mathilde\" \/><\/a><\/figure><\/div><div class=\"rttm-content-area rt-col-sm-10 rt-col-xs-8 \"><h3><span class=\"team-name\"><a class=\"\" data-id=\"17669\" target=\"_self\" title=\"SCHUCHARD Mathilde\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/schuchard-mathilde\/\">SCHUCHARD Mathilde<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"17669\" target=\"_self\" title=\"SCHUCHARD Mathilde\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/schuchard-mathilde\/\">PhD Student<\/a><\/div><div class=\"contact-info\"><ul><li class=\"tlp-location\"><i class=\"fa fa-map-marker\"><\/i><span class=\"tlp-location\">Grenoble<\/span><\/li><\/ul><\/div><\/div><\/div><\/div><div class=\"rt-col-md-6 rt-col-sm-6 rt-col-xs-12  even-grid-item rt-grid-item\" data-id=\"17719\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"17719\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/vignolles-david\/\"><img loading=\"lazy\" decoding=\"async\" width=\"225\" height=\"300\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2024\/09\/david2-rotated-e1583511464563-225x300-1.jpg\" class=\"img-responsive rt-team-img\" alt=\"VIGNOLLES David\" \/><\/a><\/figure><\/div><div class=\"rttm-content-area rt-col-sm-10 rt-col-xs-8 \"><h3><span class=\"team-name\"><a class=\"\" data-id=\"17719\" target=\"_self\" title=\"VIGNOLLES David\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/vignolles-david\/\">VIGNOLLES David<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"17719\" target=\"_self\" title=\"VIGNOLLES David\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/vignolles-david\/\">Professor<\/a><\/div><div class=\"contact-info\"><ul><li class=\"tlp-location\"><i class=\"fa fa-map-marker\"><\/i><span class=\"tlp-location\">Toulouse<\/span><\/li><\/ul><\/div><\/div><\/div><\/div><div class=\"rt-col-md-6 rt-col-sm-6 rt-col-xs-12  even-grid-item rt-grid-item\" data-id=\"17649\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"17649\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/vinograd-igor\/\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"300\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/05\/Igor_VINOGRAD.jpg\" class=\"img-responsive rt-team-img\" alt=\"VINOGRAD Igor\" \/><\/a><\/figure><\/div><div class=\"rttm-content-area rt-col-sm-10 rt-col-xs-8 \"><h3><span class=\"team-name\"><a class=\"\" data-id=\"17649\" target=\"_self\" title=\"VINOGRAD Igor\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/vinograd-igor\/\">VINOGRAD Igor<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"17649\" target=\"_self\" title=\"VINOGRAD Igor\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/vinograd-igor\/\">Researcher<\/a><\/div><div class=\"contact-info\"><ul><li class=\"tlp-location\"><i class=\"fa fa-map-marker\"><\/i><span class=\"tlp-location\">Grenoble<\/span><\/li><\/ul><\/div><\/div><\/div><\/div><div class=\"rt-loading-overlay\"><\/div><div class=\"rt-loading rt-ball-clip-rotate\"><div><\/div><\/div><\/div><\/div>[\/et_pb_code][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=&#8221;1&#8243; fullwidth=&#8221;on&#8221; admin_label=&#8221;Actus&#8221; module_id=&#8221;actualites&#8221; _builder_version=&#8221;4.27.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][\/et_pb_section][et_pb_section fb_built=&#8221;1&#8243; admin_label=&#8221;Th\u00e8mes de recherche&#8221; module_id=&#8221;themes&#8221; _builder_version=&#8221;4.27.0&#8243; _module_preset=&#8221;default&#8221; background_color=&#8221;rgba(0,0,0,0.02)&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_row _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_text _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<h3>Topics<\/h3>\n<p>[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=&#8221;1_4,3_4&#8243; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; module_alignment=&#8221;center&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;1_4&#8243; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_image src=&#8221;https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/02\/cuprate_diag.png&#8221; title_text=&#8221;cuprate_diag&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; width=&#8221;300px&#8221; width_tablet=&#8221;150%&#8221; width_phone=&#8221;150%&#8221; width_last_edited=&#8221;on|tablet&#8221; height=&#8221;300px&#8221; height_tablet=&#8221;150px&#8221; height_phone=&#8221;150px&#8221; height_last_edited=&#8221;on|desktop&#8221; global_colors_info=&#8221;{}&#8221; max_width__hover_enabled=&#8221;off|desktop&#8221; max_height__hover_enabled=&#8221;off|desktop&#8221;][\/et_pb_image][\/et_pb_column][et_pb_column type=&#8221;3_4&#8243; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_text _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p>High-Tc cuprate superconductors have the highest known superconducting critical temperature at ambient pressure. Their phase diagram features several baffling mysteries. The basic questions we are trying to answer are: what is the organizing principle of the phase diagram of high-Tc cuprates? what is the mechanism for high-Tc superconductivity? We use high magnetic fields to suppress superconductivity in order to reach and determine the nature of the electronic interactions at play in the phase diagram and in the pairing mechanism of those systems.<\/p>\n<p>[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row column_structure=&#8221;1_4,3_4&#8243; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; module_alignment=&#8221;center&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;1_4&#8243; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_image src=&#8221;https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/02\/iron_based_superconductors-2.png&#8221; title_text=&#8221;iron_based_superconductors&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; width=&#8221;300px&#8221; width_tablet=&#8221;150%&#8221; width_phone=&#8221;150%&#8221; width_last_edited=&#8221;on|tablet&#8221; height=&#8221;300px&#8221; height_tablet=&#8221;150px&#8221; height_phone=&#8221;150px&#8221; height_last_edited=&#8221;on|desktop&#8221; global_colors_info=&#8221;{}&#8221; max_width__hover_enabled=&#8221;off|desktop&#8221; max_height__hover_enabled=&#8221;off|desktop&#8221;][\/et_pb_image][\/et_pb_column][et_pb_column type=&#8221;3_4&#8243; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_text _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; link_option_url=&#8221;https:\/\/www.nature.com\/articles\/s41535-020-00295-1&#8243; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p>Iron-based superconductors form another family of superconducting materials with relatively high Tcs. Iron-based materials are usually magnets and were not known to be superconducting before the discovery of LaOFeAs in 2008. How the spins\u00a0 on iron contribute to superconductivity is actively studied. The multi-orbital physics of these materials adds another layer of complexity. By applying external forces, such as uniaxial stress, the balance of the orbital occupancy can be modified. Whether oribital fluctuations contribute to the pairing mechanism is an open question.<\/p>\n<p><span style=\"font-size: 14px\">Image :\u00a0<a href=\"https:\/\/www.nature.com\/articles\/s41535-020-00295-1\">npj Quantum Materials 5, 93 (2020)<\/a><\/span><\/p>\n<p>[\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=&#8221;1&#8243; admin_label=&#8221;Voir les posts&#8221; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_row _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_button button_url=&#8221;https:\/\/lncmi.cnrs.fr\/category\/fermions-fortement-correles&#8221; button_text=&#8221;See all articles&#8221; button_alignment=&#8221;center&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; custom_button=&#8221;on&#8221; button_text_size=&#8221;16px&#8221; global_colors_info=&#8221;{}&#8221;][\/et_pb_button][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=&#8221;1&#8243; module_id=&#8221;techniques&#8221; _builder_version=&#8221;4.27.0&#8243; _module_preset=&#8221;default&#8221; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_row _builder_version=&#8221;4.26.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;4.26.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_text module_id=&#8221;techniques&#8221; _builder_version=&#8221;4.26.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<h1 class=\"entry-title\">Techniques<\/h1>\n<p>[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row _builder_version=&#8221;4.27.2&#8243; _module_preset=&#8221;default&#8221; hover_enabled=&#8221;0&#8243; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221; sticky_enabled=&#8221;0&#8243;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;4.27.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_toggle title=&#8221;Cantilever magnetization measurement (Toulouse Contact : C. Proust, D. Vignolles)&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; hover_enabled=&#8221;0&#8243; global_colors_info=&#8221;{}&#8221; sticky_enabled=&#8221;0&#8243;]<\/p>\n<div id=\"pl-gb2659-67121f4eb3480\" class=\"panel-layout\">\n<div id=\"pg-gb2659-67121f4eb3480-0\" class=\"panel-grid panel-no-style\">\n<div id=\"pgc-gb2659-67121f4eb3480-0-0\" class=\"panel-grid-cell\">\n<div id=\"panel-gb2659-67121f4eb3480-0-0-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child\" data-index=\"0\">\n<div class=\"so-widget-sow-editor so-widget-sow-editor-base\">\n<div class=\"siteorigin-widget-tinymce textwidget\">\n<div id=\"pg-gb2718-67b2f21f4e552-1\" class=\"panel-grid panel-no-style\">\n<div id=\"pgc-gb2718-67b2f21f4e552-1-0\" class=\"panel-grid-cell\">\n<div id=\"panel-gb2718-67b2f21f4e552-1-0-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child\" data-index=\"2\">\n<div class=\"panel-widget-style panel-widget-style-for-gb2718-67b2f21f4e552-1-0-0\">\n<div class=\"so-widget-sow-editor so-widget-sow-editor-base\">\n<div class=\"siteorigin-widget-tinymce textwidget\">\n<p><a href=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/torque_schema-1.png\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/torque_schema-1.png\" width=\"660\" height=\"232\" alt=\"\" class=\"wp-image-23158 aligncenter size-full\" style=\"display: block; margin-left: auto; margin-right: auto;\" srcset=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/torque_schema-1.png 660w, https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/torque_schema-1-480x169.png 480w\" sizes=\"(min-width: 0px) and (max-width: 480px) 480px, (min-width: 481px) 660px, 100vw\" \/><\/a><\/p>\n<p>Torque magnetometry is a powerfull technique to measure quantum oscillations in metals. In pulsed field magnetic torque measurement is performed with a commercial piezoresistive micro-cantilever, as shown in the figure above. The size of the sample studied is approximately 0.1\u00d70.1\u00d70.05 mm<sup>3<\/sup>. Variations of the cantilever piezoresistance are measured with a Wheatstone bridge with an ac excitation at a frequency of 63kHz. In static field, the bending of a CuBe cantilever is measured capacitively.<\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<div id=\"pg-gb2718-67b2f21f4e552-2\" class=\"panel-grid panel-no-style\">\n<div id=\"pgc-gb2718-67b2f21f4e552-2-0\" class=\"panel-grid-cell\">\n<div id=\"panel-gb2718-67b2f21f4e552-2-0-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child\" data-index=\"3\">\n<div class=\"so-widget-sow-editor so-widget-sow-editor-base\">\n<div class=\"siteorigin-widget-tinymce textwidget\">\n<p>As an example we show quantum oscillations signal measured with torque magnetometry in pulsed field in an organic conductor \u03ba-(BEDT-TTF)2Cu(NCS)2 (left) and in a high-Tc cuprate superconductor YBa2Cu3Oy (right).<\/p>\n<p><a href=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/torque_example.png\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/torque_example.png\" width=\"564\" height=\"292\" alt=\"\" class=\"wp-image-23156 aligncenter size-full\" style=\"display: block; margin-left: auto; margin-right: auto;\" \/><\/a><\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<p>[\/et_pb_toggle][et_pb_toggle title=&#8221;Ultrasonic measurement (Grenoble contact : D. Leboeuf, Toulouse contact : C. Proust)&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; hover_enabled=&#8221;0&#8243; global_colors_info=&#8221;{}&#8221; sticky_enabled=&#8221;0&#8243;]<\/p>\n<div id=\"pg-gb2561-67bf4c3fdd616-1\" class=\"panel-grid panel-no-style\">\n<div id=\"pgc-gb2561-67bf4c3fdd616-1-0\" class=\"panel-grid-cell\">\n<div id=\"panel-gb2561-67bf4c3fdd616-1-0-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child\" data-index=\"2\">\n<div class=\"panel-widget-style panel-widget-style-for-gb2561-67bf4c3fdd616-1-0-0\">\n<div class=\"so-widget-sow-editor so-widget-sow-editor-base\">\n<div class=\"siteorigin-widget-tinymce textwidget\">\n<p>Ultrasound velocity is one of the most sensitive probe to phase transitions. A transducer is glued on the surface of the sample to generate an acoustic pulse. When travelling through the sample the pulse energy is absorbed by degrees of freedom causing a decay of the pulse amplitude. This decay is related to the ultrasound attenuation which is measured simultaneously with sound velocity.<\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<div id=\"pg-gb2561-67bf4c3fdd616-2\" class=\"panel-grid panel-no-style\">\n<div id=\"pgc-gb2561-67bf4c3fdd616-2-0\" class=\"panel-grid-cell\">\n<div id=\"panel-gb2561-67bf4c3fdd616-2-0-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child\" data-index=\"3\">\n<div class=\"so-widget-sow-editor so-widget-sow-editor-base\">\n<div class=\"siteorigin-widget-tinymce textwidget\">\n<p><a href=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/YBCO_US-1.png\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/YBCO_US-1.png\" width=\"578\" height=\"410\" alt=\"\" class=\"wp-image-23160 aligncenter size-full\" srcset=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/YBCO_US-1.png 578w, https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/YBCO_US-1-480x340.png 480w\" sizes=\"(min-width: 0px) and (max-width: 480px) 480px, (min-width: 481px) 578px, 100vw\" \/><\/a>As an example we show results of sound velocity measurements in the cuprate high-Tc YBCO. The field dependence of the sound velocity of a longitudinal mode in YBCO with doping level<span>\u00a0<\/span><i>p<\/i>\u2009=\u20090.122 measured at temperatures ranging from 9.8 to 45.2\u2009K is shown. The arrows indicate the transition towars charge order onset. Curves are shifted vertically for clarity. Click<span>\u00a0<\/span><a href=\"https:\/\/www.nature.com\/articles\/s41535-018-0084-5\">here<\/a><span>\u00a0<\/span>for more details about ultrasound in YBCO.<\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<p>[\/et_pb_toggle][et_pb_toggle title=&#8221;Transport measurement (Grenoble contact : D. Leboeuf, Toulouse contact : C. Proust, D. Vignolles)&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; hover_enabled=&#8221;0&#8243; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221; sticky_enabled=&#8221;0&#8243;]<\/p>\n<div id=\"pl-gb2659-67121f4eb3480\" class=\"panel-layout\">\n<div id=\"pg-gb2659-67121f4eb3480-0\" class=\"panel-grid panel-no-style\">\n<div id=\"pgc-gb2659-67121f4eb3480-0-0\" class=\"panel-grid-cell\">\n<div id=\"panel-gb2659-67121f4eb3480-0-0-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child\" data-index=\"0\">\n<div class=\"so-widget-sow-editor so-widget-sow-editor-base\">\n<div class=\"siteorigin-widget-tinymce textwidget\">\n<div id=\"pg-gb2728-67b2f1ae70bb5-1\" class=\"panel-grid panel-no-style\">\n<div id=\"pgc-gb2728-67b2f1ae70bb5-1-0\" class=\"panel-grid-cell\">\n<div id=\"panel-gb2728-67b2f1ae70bb5-1-0-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child\" data-index=\"1\">\n<div class=\"panel-widget-style panel-widget-style-for-gb2728-67b2f1ae70bb5-1-0-0\">\n<div class=\"so-widget-sow-editor so-widget-sow-editor-base\">\n<div class=\"siteorigin-widget-tinymce textwidget\">\n<p><a href=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/Rho_schema.png\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/Rho_schema.png\" width=\"284\" height=\"269\" alt=\"\" class=\"wp-image-23150 aligncenter size-full\" \/><\/a><\/p>\n<p>Resistivity, Hall effect, magnetoresistance are measured in metals and superconductors in order to investigate the electronic structure (Shubnikov \u2013 de Haas oscillations, Hall effect), and the carrier mobility (magnetoresistance, resistivity).<\/p>\n<p>In static field, low noise lock-in measurements are performed. Several samples can be fitted on a single probe, with or without rotation stage. Transport measurements are routinely performed in pulsed magnetic field in sample with resistance as low as 1 mohm. The measurements are performed with a current excitation between 0.1 mA and 10 mA at a frequency in the range 2 \u2013 80 kHz. A high-speed acquisition system is used to digitize the reference signal (current) and the voltage drop across the sample. The data are post-analyzed with software to perform the phase comparison.<\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<div id=\"pg-gb2728-67b2f1ae70bb5-2\" class=\"panel-grid panel-no-style\">\n<div id=\"pgc-gb2728-67b2f1ae70bb5-2-0\" class=\"panel-grid-cell\">\n<div id=\"panel-gb2728-67b2f1ae70bb5-2-0-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child\" data-index=\"2\">\n<div class=\"so-widget-sow-editor so-widget-sow-editor-base\">\n<div class=\"siteorigin-widget-tinymce textwidget\">\n<p><a href=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/Rho_exemple.png\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/Rho_exemple.png\" width=\"385\" height=\"306\" alt=\"\" class=\"wp-image-23148 aligncenter size-full\" \/><\/a>Above we show the magnetoresistance measured in an overdoped cuprate high-Tc superconductor, Tl2Ba2CuO6+delta. On top of a monotonic background, a small but clearly resolved oscillatory component appears in high field. Those Shubnikov \u2013 de Haas oscillations provide pivotal information about the electronic structure of those systems. Check<span>\u00a0<\/span><a href=\"https:\/\/www.nature.com\/articles\/nature07323?error=cookies_not_supported&amp;code=6b7c2445-c480-43d1-871d-2ddf54ebd72d\">here<\/a><span>\u00a0<\/span>for more details on this study.<\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<p>[\/et_pb_toggle][et_pb_toggle title=&#8221;Non-contact transport measurement (TDO) (Toulouse contact : C. Proust, D. Vignolles)&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; hover_enabled=&#8221;0&#8243; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221; sticky_enabled=&#8221;0&#8243;]<\/p>\n<div id=\"pl-gb2659-67121f4eb3480\" class=\"panel-layout\">\n<div id=\"pg-gb2659-67121f4eb3480-0\" class=\"panel-grid panel-no-style\">\n<div id=\"pgc-gb2659-67121f4eb3480-0-0\" class=\"panel-grid-cell\">\n<div id=\"panel-gb2659-67121f4eb3480-0-0-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child\" data-index=\"0\">\n<div class=\"so-widget-sow-editor so-widget-sow-editor-base\">\n<div class=\"siteorigin-widget-tinymce textwidget\">\n<div id=\"pg-gb2710-67b2ef84ac0fb-0\" class=\"panel-grid panel-no-style\">\n<div id=\"pgc-gb2710-67b2ef84ac0fb-0-1\" class=\"panel-grid-cell\">\n<div id=\"panel-gb2710-67b2ef84ac0fb-0-1-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child\" data-index=\"1\">\n<div class=\"so-widget-sow-editor so-widget-sow-editor-base\">\n<div class=\"siteorigin-widget-tinymce textwidget\">\n<h4><a href=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/TDO_schema.png\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/TDO_schema.png\" width=\"1443\" height=\"324\" alt=\"\" class=\"wp-image-23154 aligncenter size-full\" srcset=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/TDO_schema.png 1443w, https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/TDO_schema-1280x287.png 1280w, https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/TDO_schema-980x220.png 980w, https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/TDO_schema-480x108.png 480w\" sizes=\"(min-width: 0px) and (max-width: 480px) 480px, (min-width: 481px) and (max-width: 980px) 980px, (min-width: 981px) and (max-width: 1280px) 1280px, (min-width: 1281px) 1443px, 100vw\" \/><\/a><\/h4>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<div id=\"pg-gb2710-67b2ef84ac0fb-1\" class=\"panel-grid panel-no-style\">\n<div id=\"pgc-gb2710-67b2ef84ac0fb-1-0\" class=\"panel-grid-cell\">\n<div id=\"panel-gb2710-67b2ef84ac0fb-1-0-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child\" data-index=\"2\">\n<div class=\"panel-widget-style panel-widget-style-for-gb2710-67b2ef84ac0fb-1-0-0\">\n<div class=\"so-widget-sow-editor so-widget-sow-editor-base\">\n<div class=\"siteorigin-widget-tinymce textwidget\">\n<p>Radio frequency measurement technique based on tunnel diode oscillator (TDO) is very useful for the investigation of transport properties of metalic samples with small resistance or \/and where low contact-resistance cannot\u00a0 be achieved.<\/p>\n<p>The device is a LC-tank circuit powered by a tunnel diode biased in the negative resistance region of the current-voltage characteristic. The resistivity variation of the metallic sample leads, at first order, through skin depth variation (\u2206\u03b4), to change in coil inductance. The resulting variation of the oscillator frequency can therefore be regarded as proportional to resistivity variations.<\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<div id=\"pg-gb2710-67b2ef84ac0fb-2\" class=\"panel-grid panel-no-style\">\n<div id=\"pgc-gb2710-67b2ef84ac0fb-2-0\" class=\"panel-grid-cell\">\n<div id=\"panel-gb2710-67b2ef84ac0fb-2-0-0\" class=\"so-panel widget widget_sow-editor panel-first-child panel-last-child\" data-index=\"3\">\n<div class=\"so-widget-sow-editor so-widget-sow-editor-base\">\n<div class=\"siteorigin-widget-tinymce textwidget\">\n<p><a href=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/TDO_example.png\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/TDO_example.png\" width=\"456\" height=\"267\" alt=\"\" class=\"wp-image-23152 aligncenter size-full\" \/><\/a>As an example we show quantum oscillations obtained in the organic conductor \u03ba-(BEDT-TTF)2Cu(NCS)2 measured with torque magnetometry (blue) and with TDO method (green).<\/p>\n<p>More detailed example can be found<span> here :\u00a0<\/span><a href=\"https:\/\/iopscience.iop.org\/article\/10.1209\/0295-5075\/97\/57003\">https:\/\/iopscience.iop.org\/article\/10.1209\/0295-5075\/97\/57003<\/a><\/p>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<\/div>\n<p>[\/et_pb_toggle][et_pb_toggle title=&#8221;Nuclear Magnetic Resonance (NMR) (Grenoble contacts : M.-H. Julien, I. Vinograd)&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; hover_enabled=&#8221;0&#8243; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221; sticky_enabled=&#8221;0&#8243;]<\/p>\n<p>&nbsp;<\/p>\n<p>In a typical nuclear magnetic resonance experiment (NMR), a given nuclear species is spin-polarized by a static magnetic field and driven off-equilibrium by radiofrequency pulses. The radiofrequency response of the nuclei, recorded during the return back to equilibrium, measures how the environment of the nucleus affects the polarization. Analysis of this response provides us with a wealth of information about the local electronic, magnetic and structural properties, including how they possibly vary in space and how they fluctuate with time (dynamics).<\/p>\n<p><a href=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/NMR_example.jpg\"><img loading=\"lazy\" decoding=\"async\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/07\/NMR_example.jpg\" width=\"341\" height=\"260\" alt=\"\" class=\"wp-image-23146 aligncenter size-full\" \/><\/a><\/p>\n<p>The above example shows a two-component NMR resonance of 17O nuclei that provides evidence of charge-density wave formation in the high temperature cuprate superconductor YBa<sub>2<\/sub>Cu<sub>3<\/sub>O<sub>y<\/sub> (more details <a href=\"https:\/\/www.nature.com\/articles\/ncomms3113.pdf\">here<\/a>).<\/p>\n<p><a href=\"https:\/\/nmr-lncmi.wixsite.com\/nmrgroup\">Link to the NMR group at LNCMI<\/a><\/p>\n<p>&nbsp;<\/p>\n<p>[\/et_pb_toggle][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=&#8221;1&#8243; admin_label=&#8221;Publications&#8221; module_id=&#8221;publications&#8221; _builder_version=&#8221;4.27.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_row _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_text _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<h3>Publications<\/h3>\n<p>[\/et_pb_text][\/et_pb_column][\/et_pb_row][et_pb_row _builder_version=&#8221;4.27.2&#8243; _module_preset=&#8221;default&#8221; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;4.27.2&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_toggle title=&#8221;Selected publications&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p style=\"margin-bottom: 0cm\"><span style=\"color: #666666\"><span style=\"text-decoration: none\">\u00a0<\/span><\/span>&#8211; Charge order near the antiferromagnetic quantum critical point in the trilayer high Tc cuprate HgBa2Ca2Cu3O8+\u03b4<br \/>V. Oliviero, I. Gilmutdinov, D. Vignolles, S. Benhabib, N. Bruyant, A. Forget, D. Colson, W. A. Atkinson &amp; C. Proust<br \/><a href=\"https:\/\/www.nature.com\/articles\/s41535-024-00688-6\"> npj Quantum Materials 9, 75 (2024)<\/a><\/p>\n<p>&#8211; Universal correlation between H-linear magnetoresistance and T-linear resistivity in high-temperature superconductors<br \/>J. Ayres, M. Berben, C. Duffy, R. D. H. Hinlopen, Y.-T. Hsu, A. Cuoghi, M. Leroux, I. Gilmutdinov, M. Massoudzadegan, D. Vignolles, Y. Huang, T. Kondo, T. Takeuchi, S. Friedemann, A. Carrington, C. Proust &amp; N. E. Hussey<br \/><a href=\"https:\/\/www.nature.com\/articles\/s41467-024-52564-3\"> Nature Communications 15, 8406 (2024)<\/a><\/p>\n<p>&#8211; Hidden magnetism at the pseudogap critical point of a cuprate superconductor<br \/><span style=\"color: #666666\"><span style=\"text-decoration: none\">M<\/span><span style=\"text-decoration: none\">. <\/span><span style=\"text-decoration: none\">Frachet, I<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> Vinograd, R<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> Zhou, S<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> Benhabib, S<\/span><span style=\"text-decoration: none\">h.<\/span><span style=\"text-decoration: none\"> Wu, H<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> Mayaffre, <\/span><span style=\"text-decoration: none\">S.<\/span><span style=\"text-decoration: none\"> Kr\u00e4mer, S<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> K. Ramakrishna, A<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> P. Reyes, J<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> Debray, T<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> Kurosawa, N<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> Momono, M<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> Oda, S<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> Komiya, Sh<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> Ono, M<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> Horio, J<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> Chang, C<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> Proust, D<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\"> LeBoeuf<\/span><span style=\"text-decoration: none\"> &amp;<\/span><span style=\"text-decoration: none\"> M<\/span><span style=\"text-decoration: none\">.<\/span><span style=\"text-decoration: none\">&#8211;<\/span><span style=\"text-decoration: none\">H.<\/span><span style=\"text-decoration: none\"> Julien<\/span><\/span><br \/><a href=\"https:\/\/www.nature.com\/articles\/nature16983\"> Nature Physics 16, 1064 (2020)<\/a><\/p>\n<p>&#8211; Change of carrier density at the pseudogap critical point of a cuprate superconductor<br \/>S. Badoux, W. Tabis, F. Lalibert\u00e9, G. Grissonnanche, B. Vignolle, D. Vignolles, J. B\u00e9ard, D. A. Bonn, W. N. Hardy, R. Liang, N. Doiron-Leyraud, Louis Taillefer &amp; Cyril Proust<br \/><a href=\"https:\/\/www.nature.com\/articles\/nature16983\"> Nature 531, 210 (2016)<\/a><\/p>\n<p>[\/et_pb_toggle][et_pb_toggle title=&#8221;LNCMI publications on HAL&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p><span><div class=\"wp-rss-template-container\" data-wpra-template=\"default\" data-template-ctx=\"eyJzb3VyY2VzIjoiMTA0NDMifQ==\">\n    <div class=\"wp-rss-aggregator wpra-list-template  \" data-page=\"1\">\n    \n    \n<ul class=\"wpra-item-list rss-aggregator wpra-item-list--bullets wpra-item-list--default\"\n    start=\"1\">\n                        <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-05404414v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-05404414] First observation of quantum oscillations by transport measurements in semi-destructive pulsed magnetic fields up to 125 T<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2025-12-08\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-04787647v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04787647] Charge order near the antiferromagnetic quantum critical point in the trilayer high Tc cuprate HgBa2Ca2Cu3O8+\u03b4<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2024-11-17\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-04787643v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04787643] Universal correlation between H-linear magnetoresistance and T-linear resistivity in high-temperature superconductors<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2024-11-17\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-01719714\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01719714] Change of carrier density at the pseudogap critical point of a cuprate superconductor<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2023-11-24\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-01719714v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01719714] Change of carrier density at the pseudogap critical point of a cuprate superconductor<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2023-11-24\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-04292674\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04292674] Electrons with Planckian scattering obey standard orbital motion in a magnetic field<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2023-11-17\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-04292674v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04292674] Electrons with Planckian scattering obey standard orbital motion in a magnetic field<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2023-11-17\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-03853086\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03853086] From Low-Field Sondheimer Oscillations to High-Field Very Large and Linear Magnetoresistance in a SrTiO 3 -Based Two-Dimensional Electron Gas<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2022-11-16\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-03798442\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03798442] Magnetic freeze-out and anomalous Hall effect in ZrTe5<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2022-10-05\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-03787197\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03787197] Edwards-Anderson parameter and local Ising nematicity in FeSe revealed via NMR spectral broadening<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2022-09-24\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-03787189v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03787189] Singular magnetic anisotropy in the nematic phase of FeSe<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2022-09-24\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-02008805\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02008805] Critical Doping for the Onset of Fermi-Surface Reconstruction by Charge-Density-Wave Order in the Cuprate Superconductor La 2 \u2212 x Sr x CuO 4<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2022-05-11\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-03630224\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03630224] Magnetotransport signatures of antiferromagnetism coexisting with charge order in the trilayer cuprate HgBa2Ca2Cu3O8+\u03b4<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2022-04-05\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-03630224v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03630224] Magnetotransport signatures of antiferromagnetism coexisting with charge order in the trilayer cuprate HgBa2Ca2Cu3O8+\u03b4<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2022-04-05\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-01726828\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01726828] Inverse correlation between quasiparticle mass and Tc in a cuprate high-Tc superconductor<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2021-01-26\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-01726828v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01726828] Inverse correlation between quasiparticle mass and Tc in a cuprate high-Tc superconductor<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2021-01-26\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-03063972\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03063972] Wide critical fluctuations of the field-induced phase transition in graphite<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2020-12-14\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-03060549\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03060549] Ultrasound evidence for a two-component superconducting order parameter in Sr2RuO4<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2020-12-14\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-02264905\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02264905] New insights on frequency combinations and \u2018forbidden frequencies\u2019 in the de Haas\u2013van Alphen spectrum of \u03ba -(ET) 2 Cu(SCN) 2<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-08-07\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-01166810v2\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01166810] Non-Lifshitz-Kosevich field-and temperature-dependent amplitude of quantum oscillations in the quasi-two dimensional metal \u03b8-(ET) 4 ZnBr 4 (C 6 H 4 Cl 2 )<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-06-18\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/cea.hal.science\/cea-02086419\" target=\"_blank\" rel=\"nofollow\" class=\"\">[cea-02086419] Universal $T$-linear resistivity and Planckian dissipation in overdoped cuprates<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-04-01\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-02008799\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02008799] Quantum interference in a macroscopic van der Waals conductor<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-02-05\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-01992207\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992207] Thermodynamic phase diagram of static charge order in underdoped YBa2Cu3O y<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-01-24\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-01707309\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01707309] Anomalous critical fields in quantum critical superconductors<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2018-02-12\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-01707309v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01707309] Anomalous critical fields in quantum critical superconductors<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2018-02-12\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00938390\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00938390] Universal quantum oscillations in the underdoped cuprate superconductors<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2014-01-29\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00877970\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00877970] Quasiparticle Mass Enhancement Close to the Quantum Critical Point in BaFe2(As1xPx)2<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2013-10-29\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00877970v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00877970] Quasiparticle Mass Enhancement Close to the Quantum Critical Point in BaFe2(As1xPx)2<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2013-10-29\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00804863\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00804863] From quantum oscillations to charge order in high-copper oxides in high magnetic fields<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2013-03-26\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00804863v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00804863] From quantum oscillations to charge order in high-copper oxides in high magnetic fields<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2013-03-26\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00755646\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00755646] Vortex lattice melting and Hc2 in underdoped YBa2Cu3Oy<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2012-11-21\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00755646v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00755646] Vortex lattice melting and Hc2 in underdoped YBa2Cu3Oy<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2012-11-21\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00727411v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00727411] Coherent c-axis transport in the underdoped cuprate superconductor YBCO<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2012-09-03\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00633166v3\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00633166] Quantum oscillations in the linear chain of coupled orbits: the organic metal with two cation layers theta-(ET)(4)CoBr(4)(C(6)H(4)Cl(2))<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2012-02-03\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00655990\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00655990] Quantum oscillations and the Fermi surface of high-temperature cuprate superconductors<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2012-01-03\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00655990v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00655990] Quantum oscillations and the Fermi surface of high-temperature cuprate superconductors<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2012-01-03\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00643286\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00643286] Fermi-surface reconstruction by stripe order in cuprate superconductors<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2011-11-21\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00609914\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00609914] Phase-fluctuating superconductivity in overdoped La2-xSrxCuO4<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2011-07-20\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00608272\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00608272] Fermi surface of the electron-doped cuprate superconductor Nd2xCexCuO4 probed by high-field magnetotransport<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2011-07-12\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00608272v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00608272] Fermi surface of the electron-doped cuprate superconductor Nd2xCexCuO4 probed by high-field magnetotransport<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2011-07-12\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00595071\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00595071] Temperature- and pressure-dependent metallic states in (BEDT-TTF)8[Hg4Br12(C6H5Br)2]<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2011-05-27\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00577853\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00577853] Angle dependence of quantum oscillations in YBa2Cu3O6.59 shows free-spin behaviour of quasiparticles<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2011-03-17\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00458187\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00458187] Evolution of the Fermi Surface of BaFe2 (As1-xPx)2 on Entering the Superconducting Dome<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2010-02-19\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00458187v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00458187] Evolution of the Fermi Surface of BaFe2 (As1-xPx)2 on Entering the Superconducting Dome<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2010-02-19\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00441724\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00441724] On the destruction of the hidden order in URu2Si2 by a strong magnetic field<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2009-12-17\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00441073\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00441073] Quantum oscillations in underdoped YBa2Cu3O6:5.<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2009-12-14\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00441073v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00441073] Quantum oscillations in underdoped YBa2Cu3O6:5.<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2009-12-14\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00441001\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00441001] Multiple quantum oscillations in the de Haas-van Alphen spectra of the underdoped high-temperature superconductor YBa2Cu3O6:5<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2009-12-14\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00441001v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00441001] Multiple quantum oscillations in the de Haas-van Alphen spectra of the underdoped high-temperature superconductor YBa2Cu3O6:5<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2009-12-14\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00355122\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00355122] de Haas-van Alphen Oscillations in the Underdoped High-Temperature Superconductor YBa2Cu3O6.5<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2009-01-22\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00355122v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00355122] de Haas-van Alphen Oscillations in the Underdoped High-Temperature Superconductor YBa2Cu3O6.5<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2009-01-22\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00355119\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00355119] Skutterudite Results Shed Light on Heavy Fermion Physics<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2009-01-22\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00222080\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00222080] Quantum oscillations and Fermi surface in YBa2Cu3O6.5<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-01-29\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00222080v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00222080] Quantum oscillations and Fermi surface in YBa2Cu3O6.5<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-01-29\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00222074v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00222074] Fermi surface of underdoped cuprate revealed by quantum oscillations and Hall effect<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-01-29\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00222052\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00222052] Fermi surface of underdoped cuprate revealed by quantum oscillations and Hall effect<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-01-29\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00222052v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00222052] Fermi surface of underdoped cuprate revealed by quantum oscillations and Hall effect<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-01-29\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00222035\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00222035] Quantum oscillations and the Fermi surface in underdoped high-Tc superconductors<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-01-29\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00222035v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00222035] Quantum oscillations and the Fermi surface in underdoped high-Tc superconductors<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-01-29\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00222018\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00222018] Surface de Fermi r\u00e9v\u00e9l\u00e9e par des oscillations quantiques dans YBa2Cu306.5<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-01-29\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00222018v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00222018] Surface de Fermi r\u00e9v\u00e9l\u00e9e par des oscillations quantiques dans YBa2Cu306.5<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-01-29\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00207140\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00207140] Syst\u00e8mes fortement corr\u00e9l\u00e9s : diagramme de phase, criticalit\u00e9 et fermiologie<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-01-17\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00207140v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00207140] Syst\u00e8mes fortement corr\u00e9l\u00e9s : diagramme de phase, criticalit\u00e9 et fermiologie<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-01-17\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00207060\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00207060] Oscillations de Haas-van Alphen dans le compos\u00e9 \u00e0 fermions lourds CeCoIn5<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-01-17\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00207060v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00207060] Oscillations de Haas-van Alphen dans le compos\u00e9 \u00e0 fermions lourds CeCoIn5<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-01-17\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00124165\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00124165] Metallic ground state in underdoped YBa2Cu3Oy<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2007-01-12\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00124165v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00124165] Metallic ground state in underdoped YBa2Cu3Oy<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2007-01-12\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/inria.hal.science\/inria-00108094\" target=\"_blank\" rel=\"nofollow\" class=\"\">[inria-00108094] Mod\u00e8les et Algorithmes en Ordonnancement: Exercices et Probl\u00e8mes Corrig\u00e9s<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2006-10-19\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00017083\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00017083] Supraconductivit\u00e9 et instabilit\u00e9 \u00e9lectronique sous champ magn\u00e9tique intense<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2006-02-09\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00017083v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00017083] Supraconductivit\u00e9 et instabilit\u00e9 \u00e9lectronique sous champ magn\u00e9tique intense<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2006-02-09\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00018320\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00018320] Magnetic oscillations in a two-dimensional network of coupled orbits<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2006-01-31\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00018320v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00018320] Magnetic oscillations in a two-dimensional network of coupled orbits<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2006-01-31\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00015949\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00015949] Magnetic oscillations in a two-dimensional network of compensated electron and hole orbits<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2006-01-27\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00015760\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00015760] Low temperature physics at the Laboratoire National des Champs Magn\u00e9tiques Puls\u00e9s in Toulouse<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2006-01-25\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00015760v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00015760] Low temperature physics at the Laboratoire National des Champs Magn\u00e9tiques Puls\u00e9s in Toulouse<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2006-01-25\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00014428\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00014428] Magnetic oscillations in the two-dimensional network of coupled orbits of the organic metals (BEDT-TTF)8Hg4Cl12(C6H5X)2 (X = Cl, Br)<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2006-01-18\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n                    <li class=\"wpra-item feed-item \">\n            \n            \n\n    <a  href=\"https:\/\/hal.science\/hal-00014428v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00014428] Magnetic oscillations in the two-dimensional network of coupled orbits of the organic metals (BEDT-TTF)8Hg4Cl12(C6H5X)2 (X = Cl, Br)<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2006-01-18\n        <\/span>\n    \n    <\/div>\n\n\n\n\n\n            \n        <\/li>\n        <\/ul>\n\n        \n<\/div>\n\n<\/div>\n<\/span><\/p>\n<p>[\/et_pb_toggle][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=&#8221;1&#8243; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_row _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_column type=&#8221;4_4&#8243; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=&#8221;1&#8243; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_row _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; 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[&hellip;]<\/p>\n","protected":false},"author":12,"featured_media":10412,"parent":18218,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"_et_pb_use_builder":"on","_et_pb_old_content":"","_et_gb_content_width":"","footnotes":""},"folder":[182],"class_list":["post-10411","page","type-page","status-publish","has-post-thumbnail","hentry"],"jetpack_sharing_enabled":true,"_links":{"self":[{"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/pages\/10411","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/users\/12"}],"replies":[{"embeddable":true,"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/comments?post=10411"}],"version-history":[{"count":0,"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/pages\/10411\/revisions"}],"up":[{"embeddable":true,"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/pages\/18218"}],"wp:featuredmedia":[{"embeddable":true,"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/media\/10412"}],"wp:attachment":[{"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/media?parent=10411"}],"wp:term":[{"taxonomy":"folder","embeddable":true,"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/folder?post=10411"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}