{"id":10415,"date":"2024-06-28T15:57:43","date_gmt":"2024-06-28T13:57:43","guid":{"rendered":"https:\/\/lncmi.cnrs.fr\/?page_id=9854"},"modified":"2025-05-26T14:04:47","modified_gmt":"2025-05-26T12:04:47","slug":"nmr-of-unconventional-electronic-materials","status":"publish","type":"page","link":"https:\/\/lncmi.cnrs.fr\/en\/highly-correlated-electronic-systems\/nmr-of-unconventional-electronic-materials\/","title":{"rendered":"NMR of unconventional electronic materials"},"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\/gros-plan-neons-colores-abstraits-perspective-parfaits-pour-concept-scifi_181624-56907.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; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; sticky_position=&#8221;top&#8221; hover_enabled=&#8221;0&#8243; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221; disabled_on=&#8221;on|off|off&#8221; sticky_enabled=&#8221;0&#8243;][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; _builder_version=&#8221;4.27.2&#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;#personnel&#8221; button_text=&#8221;Staff&#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;#actualites&#8221; button_text=&#8221;Features&#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;#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;Description&#8221; module_id=&#8221;description&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; min_height=&#8221;580.5px&#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;4.25.2&#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>Exploring Unconventional Electronic Materials with NMR<\/h3>\n<p>[\/et_pb_text][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<div id=\"bgLayers_comp-ld35j1d31\" data-hook=\"bgLayers\" data-motion-part=\"BG_LAYER\" class=\"MW5IWV\">\n<div id=\"bgMedia_comp-ld35j1d31\" data-motion-part=\"BG_MEDIA\" class=\"VgO9Yg\" style=\"text-align: justify\">\n<p data-start=\"214\" data-end=\"350\" class=\"\">We use <strong data-start=\"221\" data-end=\"257\">nuclear magnetic resonance (NMR)<\/strong> to investigate materials with unconventional electronic properties at the microscopic scale.<\/p>\n<p data-start=\"352\" data-end=\"648\" class=\"\">NMR, a technique based on the same physical principles as magnetic resonance imaging (MRI), employs atomic nuclei as <strong data-start=\"469\" data-end=\"485\">local probes<\/strong> of matter. This allows us to uncover rich information about the <strong data-start=\"550\" data-end=\"606\">electronic, magnetic, and structural properties<\/strong> of materials with atomic-level precision.<\/p>\n<p data-start=\"650\" data-end=\"674\" class=\"\">Our research focuses on:<\/p>\n<ul data-start=\"676\" data-end=\"1182\">\n<li data-start=\"676\" data-end=\"858\" class=\"\">\n<p data-start=\"678\" data-end=\"858\" class=\"\"><strong data-start=\"678\" data-end=\"712\">Unconventional superconductors<\/strong>, including high-temperature cuprate and iron-based families, as well as exotic superconducting states that emerge under strong magnetic fields.<\/p>\n<\/li>\n<li data-start=\"859\" data-end=\"976\" class=\"\">\n<p data-start=\"861\" data-end=\"976\" class=\"\"><strong data-start=\"861\" data-end=\"889\">Unconventional magnetic systems<\/strong>, such as <strong data-start=\"899\" data-end=\"930\">one-dimensional spin chains<\/strong> and <strong data-start=\"935\" data-end=\"973\">frustrated two-dimensional magnets<\/strong>.<\/p>\n<\/li>\n<li data-start=\"977\" data-end=\"1107\" class=\"\">\n<p data-start=\"979\" data-end=\"1107\" class=\"\"><strong data-start=\"979\" data-end=\"1011\">Complex electronic phases<\/strong>, including <strong data-start=\"1023\" data-end=\"1047\">charge-density waves<\/strong>, <strong data-start=\"1049\" data-end=\"1074\">electronic nematicity<\/strong>, and <strong data-start=\"1080\" data-end=\"1104\">the fascinating effects of disorder<\/strong>.<\/p>\n<\/li>\n<li data-start=\"1108\" data-end=\"1182\" class=\"\">\n<p data-start=\"1110\" data-end=\"1182\" class=\"\">A range of magnetically interesting molecules.<\/p>\n<\/li>\n<\/ul>\n<p data-start=\"1184\" data-end=\"1478\" class=\"\">A distinctive feature of our research is the use of <strong data-start=\"1125\" data-end=\"1154\">very high magnetic fields<\/strong>, generated by superconducting or resistive magnets. These fields often uncover hidden phases or induce dramatic changes in material behavior, enabling us to <strong data-start=\"1312\" data-end=\"1364\">tune and understand their fundamental properties<\/strong>.<\/p>\n<p data-start=\"1184\" data-end=\"1478\" class=\"\">\n<p data-start=\"1184\" data-end=\"1478\" class=\"\">More information on the <a href=\"https:\/\/nmr-lncmi.wixsite.com\/nmrgroup\" target=\"_blank\" rel=\"noopener\">group website<\/a><\/p>\n<\/div>\n<\/div>\n<\/div>\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;Annuaire&#8221; module_id=&#8221;personnel&#8221; _builder_version=&#8221;4.26.0&#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;4.26.0&#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-10472' id='rt-team-container-2574308544'  data-layout='layout2' data-desktop-col='2'  data-tab-col='2'  data-mobile-col='1' data-sc-id='10472' 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=\"24248\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"24248\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/costarella-benjamin\/\"><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=\"24248\" target=\"_self\" title=\"COSTARELLA Benjamin\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/costarella-benjamin\/\">COSTARELLA Benjamin<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"24248\" target=\"_self\" title=\"COSTARELLA Benjamin\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/costarella-benjamin\/\">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=\"17735\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"17735\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/horvatic-mladen\/\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"300\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/05\/Mladen_HORVATIC.jpg\" class=\"img-responsive rt-team-img\" alt=\"HORVATIC Mladen\" \/><\/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=\"17735\" target=\"_self\" title=\"HORVATIC Mladen\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/horvatic-mladen\/\">HORVATIC Mladen<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"17735\" target=\"_self\" title=\"HORVATIC Mladen\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/horvatic-mladen\/\">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=\"20860\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"20860\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/julien-marc-henri\/\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"300\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/05\/Marc-henri_Julien.jpg\" class=\"img-responsive rt-team-img\" alt=\"JULIEN Marc-Henri\" \/><\/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=\"20860\" target=\"_self\" title=\"JULIEN Marc-Henri\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/julien-marc-henri\/\">JULIEN Marc-Henri<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"20860\" target=\"_self\" title=\"JULIEN Marc-Henri\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/julien-marc-henri\/\">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=\"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=\"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;4.26.0&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][et_pb_fullwidth_post_slider posts_number=&#8221;5&#8243; include_categories=&#8221;2712,2805&#8243; excerpt_length=&#8221;100&#8243; show_meta=&#8221;off&#8221; use_text_overlay=&#8221;off&#8221; _builder_version=&#8221;4.26.0&#8243; _module_preset=&#8221;default&#8221; header_font=&#8221;|700|on||||||&#8221; header_text_align=&#8221;left&#8221; body_font=&#8221;&#8211;et_global_body_font||||||||&#8221; body_text_align=&#8221;left&#8221; body_line_height=&#8221;1.4em&#8221; background_color=&#8221;#FFFFFF&#8221; custom_button=&#8221;on&#8221; button_border_radius=&#8221;100px&#8221; button_font=&#8221;Verdana||||||||&#8221; button_alignment=&#8221;left&#8221; width=&#8221;70%&#8221; module_alignment=&#8221;center&#8221; content_width=&#8221;100%&#8221; height=&#8221;300px&#8221; height_tablet=&#8221;300px&#8221; height_phone=&#8221;350px&#8221; height_last_edited=&#8221;on|phone&#8221; max_height=&#8221;300px&#8221; max_height_tablet=&#8221;300px&#8221; max_height_phone=&#8221;350px&#8221; max_height_last_edited=&#8221;on|desktop&#8221; custom_margin=&#8221;25px|25px|25px|25px|true|true&#8221; custom_padding=&#8221;60px||74px||false|false&#8221; auto=&#8221;on&#8221; auto_speed=&#8221;10000&#8243; hover_transition_duration=&#8221;500ms&#8221; hover_transition_speed_curve=&#8221;ease-in&#8221; body_font_size_tablet=&#8221;&#8221; body_font_size_phone=&#8221;15px&#8221; body_font_size_last_edited=&#8221;on|phone&#8221; button_text_size_tablet=&#8221;17px&#8221; button_text_size_phone=&#8221;14px&#8221; button_text_size_last_edited=&#8221;on|tablet&#8221; custom_css_free_form=&#8221;.et_pb_more_button:hover{||  -webkit-backdrop-filter: blur(5px);||  backdrop-filter: blur(5px);||  border: solid 2px rgba(255,255,255,0.2) !IMPORTANT;||  transition: backdrop-filter ease-in-out 0.2s;||}&#8221; header_text_shadow_style=&#8221;preset1&#8243; header_text_shadow_blur_strength=&#8221;1em&#8221; border_radii=&#8221;on|25px|25px|25px|25px&#8221; border_color_all=&#8221;#FFFFFF&#8221; button_text_shadow_style=&#8221;preset1&#8243; button_text_shadow_blur_strength=&#8221;1em&#8221; box_shadow_style=&#8221;preset3&#8243; box_shadow_blur=&#8221;23px&#8221; box_shadow_spread=&#8221;-30px&#8221; box_shadow_style_button=&#8221;preset1&#8243; global_colors_info=&#8221;{}&#8221; box_shadow_blur__hover_enabled=&#8221;on|desktop&#8221; box_shadow_vertical__hover_enabled=&#8221;on|hover&#8221; box_shadow_vertical__hover=&#8221;10px&#8221; box_shadow_blur__hover=&#8221;25px&#8221; box_shadow_spread__hover=&#8221;-10px&#8221; box_shadow_spread__hover_enabled=&#8221;on|hover&#8221;][\/et_pb_fullwidth_post_slider][\/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\/aimants-quantiques-et-frustres-par-rmn&#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; _builder_version=&#8221;4.26.0&#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; 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;High-field and high-frequency NMR&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p><strong>Nuclear Magnetic Resonance (NMR)<\/strong> is widely used for the <strong>determination of molecular structures in chemistry and biology<\/strong>, where high magnetic fields are applied to increase the sensitivity and resolution of this technique. Its applications also include the analysis of innovative and functional materials such as superconductors, magnetic components, catalysts, materials for energy storage or contrast agents for magnetic resonance imaging (MRI).<\/p>\n<p><strong>NMR at LNCMI Grenoble goes beyond the magnetic fields provided by superconducting magnets to reach 37 T<\/strong>. NMR probes with variable frequencies (up to <strong>1500 MHz<\/strong>), variable temperatures (<strong>50 mK-300 K<\/strong>) and the <strong>improved 10 ppm<\/strong> resolution required for solid-state chemistry are also available, and are the subject of ongoing development.<\/p>\n<p>LNCMI&#8217;s NMR team is available to support users in their projects.<\/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;4.27.2&#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 (last 5 years)&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p><span><strong>Spin-stripe order tied to the pseudogap phase in La1.8\u2212xEu0.2SrxCuO4<\/strong>, <\/span><span>A. Missiaen, H. Mayaffre, S. Kr\u00e4mer, D. Zhao, Y. Zhou,T. Wu, X.H. Chen, S. Pyon, T. Takayama, H. Takagi, D. LeBoeuf, M.-H. Julien, <\/span><a href=\"https:\/\/doi.org\/10.1103\/PhysRevX.15.021010\" target=\"_blank\" rel=\"noopener\">Phys. Rev. X 15, 021010 (2025)<\/a><\/p>\n<p><span>\u200b<strong>Signatures of two gaps in the spin susceptibility of a cuprate superconductor<\/strong>, R. <\/span><span>Zhou, M. Hirata, I. Vinograd, T. Wu, H. Mayaffre, S. Kr\u00e4mer, R. Liang, W. N. Hardy, D. A. Bonn, T. Loew, J. Porras, B. Keimer, M.-H. Julien,<\/span><a href=\"https:\/\/doi.org\/10.1038\/s41567-024-02692-w\" target=\"_blank\" rel=\"noopener\"> Nature Physics <strong>21<\/strong>,\u00a0 97 (2025)<\/a>.<\/p>\n<p><span><strong>Narrowly avoided spin-nematic phase in BaCdVO(PO4)2: NMR evidence<\/strong>, <\/span><span>M. Ranjith, K. Yu. Povarov, Z. Yan, A. Zheludev, M. Horvati\u0107,\u00a0<\/span><span><a href=\"https:\/\/doi.org\/10.1103\/PhysRevResearch.6.023043\">Phys. Rev. Research 6, 023043 (2024)<\/a>.<\/span><\/p>\n<p><span><strong>Magnetic and structural properties of the iron silicide superconductor LaFeSiH<\/strong>, M.<\/span><span>F. Hansen, S. Layek, J.-B. Vaney, L. Chaix, M. R. Suchomel, M. Mikolasek, G. Gar- barino, A. Chumakov, R. R\u00fcffer, V. Nassif, T. Hansen, E. Elkaim, T. Pelletier, H. Mayaffre, F. Bernardini, A. Sulpice, M. N\u00fa\u00f1ez-Regueiro, P. Rodi\u00e8re, A. Cano, S. Tenc\u00e9, P. Toulemonde, M.-H. Julien, and M. d\u2019Astuto, <\/span><span><a href=\"https:\/\/doi.org\/10.1103\/PhysRevB.109.1\" target=\"_blank\" rel=\"noopener\">Phys. Rev. B 109, 174523 (2024)<\/a>.<\/span><\/p>\n<p><span><strong>Longitudinal Spin Fluctuations Driving Field-Reinforced Superconductivity in UTe2<\/strong>,\u00a0Y. Tokunaga, H. Sakai, S. Kambe, P. Opletal, Y. Tokiwa, Y. Haga, S. Kitagawa, K. Ishida, D. Aoki, G. Knebel, G. Lapertot, S. Kr\u00e4mer, and M. Horvati\u0107, <a href=\"https:\/\/doi.org\/10.1103\/PhysRevLett.131.226503\">Phys. Rev. Lett. 131, 226503 (2023).<\/a><\/span><\/p>\n<p><span><strong>Second order Zeeman interaction and ferroquadrupolar order in TmVO4<\/strong>, <\/span><span>I. Vinograd, K. R. Shirer, P. Massat, Z. Wang, T. Kissikov, D. Garcia, M. D. Bachmann, M. Horvati\u0107, I. R. Fisher and N. J. Curro<\/span><br \/><span><a href=\"https:\/\/doi.org\/10.1038\/s41535-022-00475-1\">npj Quantum Mater. 7, 68 (2022)<\/a><\/span><\/p>\n<p><strong>Superconductivity in the crystallogenide LaFeSiO1\u2212\u03b4 with squeezed FeSi layers<\/strong>, M.F. Hansen, J.-B. Vaney, C. Lepoittevin, F. Bernardini, E. Gaudin, V. Nassif, M.-A. M\u00e9asson, A. Sulpice, H. Mayaffre, M.-H. Julien, S. Tenc\u00e9, A. Cano, and P. Toulemonde, <span><a href=\"https:\/\/doi.org\/10.1038\/s41535-022-00493-z\">npj Quantum Mater. 7, 86 (2022)<\/a><\/span>.<\/p>\n<p><span>\u200b<\/span><strong>Competition between spin ordering and superconductivity near the pseudogap boundary in La2\u2212xSrxCuO4: insights from NMR<\/strong>, I. Vinograd, R. Zhou, H. Mayaf- fre, S. Kr\u00e4mer, S. K. Ramakrishna, A. P. Reyes, T. Kurosawa, N. Momono, M. Oda, S. Komiya, S. Ono, M. Horio, J. Chang, and M.-H. Julien, <span><a href=\"https:\/\/doi.org\/10.1103\/PhysRevB.106.054522\">Phys. Rev. B 106, 054522 (2022)<\/a><\/span>. <span>\u200b<\/span><\/p>\n<p><span><strong>NMR evidence against a spin-nematic nature of the presaturation phase in the frustrated magnet SrZnVO(PO4)2<\/strong>,\u00a0 <\/span><span>K. M. Ranjith, F. Landolt, S. Raymond, A. Zheludev, and M. Horvati\u0107, <\/span><span><a href=\"https:\/\/doi.org\/10.1103\/PhysRevB.105.134429\">\u00a0Phys. Rev. B 105, 134429 (2022)<\/a>.<\/span><\/p>\n<p><span>\u200b<\/span><span><strong>Competing magnetic phases in the frustrated spin-1\/2 chain compound \u03b2\u2212TeVO4 probed by NMR<\/strong>,\u00a0 <\/span><span>M. Pregelj, A. Zorko, D. Ar\u010don, M. Klanj\u0161ek, N. Jan\u0161a, P. Jegli\u010d, O. Zaharko, S. Kr\u00e4mer, M. Horvati\u0107, and A. Prokofiev, <\/span><span><a href=\"https:\/\/doi.org\/10.1103\/PhysRevB.105.035145\">Phys. Rev. B 105, 035145 (2022)<\/a>.<\/span><\/p>\n<p><span><strong>Edwards-Anderson parameter and local Ising-nematicity in FeSe revealed via NMR spectral broadening<\/strong>, P. <\/span><span>Wiecki, R. Zhou, M.-H. Julien, A. E. B\u00f6hmer, J. Schmalian,\u00a0<\/span><span><a href=\"https:\/\/doi.org\/10.1103\/PhysRevB.104.125134\">Phys. Rev. B 104, 125134 (2021)<\/a>.<\/span><\/p>\n<p><span><strong>Revealing three-dimensional quantum criticality by Sr substitution in Han Purple<\/strong>, S. <\/span><span>Allenspach, P. Puphal, J. Link, I. Heinmaa, E. Pomjakushina, C. Krellner, J. Lass, G.S. Tucker, C. Niedermayer, S. Imajo, Y. Kohama, K. Kindo, S. Kr\u00e4mer, M. Horvati\u0107, M. Jaime, A. Madsen, A. Mira, N. Laflorencie, F. Mila, B. Normand, C. R\u00fcegg, R. Stern, and F. Weickert,\u00a0<\/span><span><a href=\"https:\/\/doi.org\/10.1103\/PhysRevResearch.3.023177\">Phys. Rev. Research 3, 023177 (2021)<\/a><\/span><span>\u200b<\/span><\/p>\n<p><span><strong>High magnetic field ultrasound study of spin freezing in La1.88Sr0.12CuO4<\/strong>, M. <\/span><span>Frachet, S. Benhabib, I. Vinograd, S.-F. Wu, B. Vignolle, H. Mayaffre, S. Kr\u00e4mer, T. Kurosawa, N. Momono, M. Oda, J. Chang, C. Proust, M.-H. Julien, and D. LeBoeuf, <\/span><span><a href=\"https:\/\/doi.org\/10.1103\/PhysRevB.103.115133\">Phys. Rev. B 103, 115133 (2021)<\/a>.<\/span><\/p>\n<p><span><strong>Locally commensurate charge-density wave with three-unit-cell periodicity in YBa2Cu3Oy<\/strong>, I. <\/span><span>Vinograd, R. Zhou, M. Hirata, T. Wu, H. Mayaffre, S. Kr\u00e4mer, R. Liang, W.N. Hardy, D.A. Bonn, and M.-H. Julien, <\/span><span><a href=\"https:\/\/doi.org\/10.1038\/s41467-021-23140-w\">Nat. Commun. 12, 3274 (2021)<\/a>.<\/span><\/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=\"eyJzb3VyY2VzIjoiMTA0NzAifQ==\">\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-05243848v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-05243848] Robust Charge Density Wave Correlations in Optimally Doped 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 2025-09-07\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-04770173v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04770173] Properties of an organic model S=1 Haldane chain system<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2024-11-06\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-04560386\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04560386] Narrowly avoided spin-nematic phase in BaCdVO(PO4)2: NMR evidence<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2024-04-26\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-04560386v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04560386] Narrowly avoided spin-nematic phase in BaCdVO(PO4)2: NMR evidence<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2024-04-26\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-04300294\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04300294] Longitudinal spin fluctuations driving field-reinforced superconductivity in UTe$_2$<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2023-11-22\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-04300294v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04300294] Longitudinal spin fluctuations driving field-reinforced superconductivity in UTe$_2$<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2023-11-22\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-03787195\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03787195] Locally commensurate charge-density wave with three-unit-cell periodicity in 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 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-03711259v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03711259] Second order Zeeman interaction and ferroquadrupolar order in TmVO4<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2022-07-01\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-03671688\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03671688] NMR evidence against a spin-nematic nature of the presaturation phase in the frustrated magnet SrZnVO(PO4)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 2022-05-18\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:\/\/ens-lyon.hal.science\/ensl-00565064\" target=\"_blank\" rel=\"nofollow\" class=\"\">[ensl-00565064] Luttinger liquid physics in the spin ladder material CuBr4(C5H12N)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 2021-04-13\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-02576102\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02576102] Field-dependent paramagnetic relaxation enhancement in solutions of Ni(II): What happens above the NMR proton frequency of 1\u202fGHz?<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2020-11-30\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-03024412\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03024412] Hidden magnetism 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 2020-11-25\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-02866081\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02866081] Direct determination of the Tomonaga-Luttinger parameter K in quasi-one-dimensional spin systems<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2020-06-12\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-02866081v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02866081] Direct determination of the Tomonaga-Luttinger parameter K in quasi-one-dimensional spin systems<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2020-06-12\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-02525703\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02525703] $^{105}$Pd NMR and NQR study of the cubic heavy fermion system Ce$_3$Pd$_{20}$Si$_6$<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2020-03-31\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-02525703v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02525703] $^{105}$Pd NMR and NQR study of the cubic heavy fermion system Ce$_3$Pd$_{20}$Si$_6$<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2020-03-31\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-02305943\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02305943] Field-angular Dependence of Pairing Interaction in URhGe: Comparison with UCoGe<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-10-04\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-02272025\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02272025] Dynamics and field-induced order in the layered spin S = 1\/2 dimer system (C5H6N2F)2CuCl4<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-08-27\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-02272025v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02272025] Dynamics and field-induced order in the layered spin S = 1\/2 dimer system (C5H6N2F)2CuCl4<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-08-27\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-01998113\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01998113] Nuclear Magnetic Resonance Signature of the Spin-Nematic Phase in LiCuVO4 at 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 2019-06-13\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-02055781\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02055781] High-field phase diagram of the heavy-fermion metal CeIn3: Pulsed-field NMR study on single crystals up to 56 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 2019-03-04\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-01998593\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01998593] C13 NMR study of the charge-ordered state near the superconducting transition in the organic superconductor \u03b2\u2032\u2032\u2212(BEDT-TTF)4[(H3O)Ga(C2O4)3]\u00b7C6H5NO2<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-01-29\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-01998593v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01998593] C13 NMR study of the charge-ordered state near the superconducting transition in the organic superconductor \u03b2\u2032\u2032\u2212(BEDT-TTF)4[(H3O)Ga(C2O4)3]\u00b7C6H5NO2<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-01-29\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-01998565\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01998565] One-Third Magnetization Plateau with a Preceding Novel Phase in Volborthite<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-01-29\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-01998097\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01998097] Competing Bose-glass physics with disorder-induced Bose-Einstein condensation in the doped S = 1 antiferromagnet Ni(Cl(1\u2212x)Br(x))2\u22124SC(NH2)2 at 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 2019-01-29\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-01998084\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01998084] Dynamics of bound magnon pairs in the quasi-one-dimensional frustrated magnet LiCuVO4<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-01-29\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-01997584\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01997584] Evidence of Andreev bound states as a hallmark of the FFLO phase in \u03ba-(BEDT-TTF) 2 Cu(NCS) 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 2019-01-29\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-01992535\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992535] Incipient charge order observed by NMR in the normal state of 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 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-01992526\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992526] Emergence of Orbital Nematicity in the Tetragonal Phase of BaFe 2 (As 1\u2212 x P x ) 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 2019-01-24\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-01992526v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992526] Emergence of Orbital Nematicity in the Tetragonal Phase of BaFe 2 (As 1\u2212 x P x ) 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 2019-01-24\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-01992505v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992505] Quantum tricritical fluctuations driving mass enhancement and reentrant superconductivity in URhGe<\/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-01992497v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992497] Interplay between quantum fluctuations and reentrant superconductivity with a highly enhanced upper critical field in URhGe<\/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-01992488\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992488] Quasiparticle Scattering off Defects and Possible Bound States in Charge-Ordered YBa 2 Cu 3 O 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-01992488v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992488] Quasiparticle Scattering off Defects and Possible Bound States in Charge-Ordered YBa 2 Cu 3 O 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-01992479\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992479] Field-induced reentrant superconductivity driven by quantum tricritical fluctuations in URhGe<\/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-01992479v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992479] Field-induced reentrant superconductivity driven by quantum tricritical fluctuations in URhGe<\/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-01985996\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01985996] Hyperfine coupling and spin polarization in the bulk of the topological insulator Bi 2 Se 3<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-01-18\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-01985996v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01985996] Hyperfine coupling and spin polarization in the bulk of the topological insulator Bi 2 Se 3<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-01-18\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-01926975\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01926975] Detection of a Disorder-Induced Bose-Einstein Condensate in a Quantum Spin Material at 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 2018-11-19\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-01926975v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01926975] Detection of a Disorder-Induced Bose-Einstein Condensate in a Quantum Spin Material at 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 2018-11-19\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:\/\/cea.hal.science\/cea-01745392\" target=\"_blank\" rel=\"nofollow\" class=\"\">[cea-01745392] Reentrant Superconductivity Driven by Quantum Tricritical Fluctuations in URhGe: Evidence from $^{59}$Co NMR in URh$_{0.9}$Co$_{0.1}$Ge<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2018-03-28\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-01478853\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01478853] Nuclear Magnetic Resonance Reveals Disordered Level-Crossing Physics in the Bose-Glass Regime of the Br-Doped Ni(Cl1\u2212xBrx)2\u22124SC(NH2)2 Compound at a High 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 2017-02-28\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-01478853v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01478853] Nuclear Magnetic Resonance Reveals Disordered Level-Crossing Physics in the Bose-Glass Regime of the Br-Doped Ni(Cl1\u2212xBrx)2\u22124SC(NH2)2 Compound at a High 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 2017-02-28\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-01472150\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01472150] Nuclear magnetic resonance study of the magnetic-field-induced ordered phase in the NiCl2\u22124SC(NH2)2 compound<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2017-02-20\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-01472150v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01472150] Nuclear magnetic resonance study of the magnetic-field-induced ordered phase in the NiCl2\u22124SC(NH2)2 compound<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2017-02-20\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:\/\/ens-lyon.hal.science\/ensl-01186120\" target=\"_blank\" rel=\"nofollow\" class=\"\">[ensl-01186120] Giant magnetic field dependence of the coupling between spin chains in BaCo2V2O8<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2015-08-24\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-00986315\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00986315] Spatially resolved magnetization in the Bose-Einstein condensed state of BaCuSi2O6: Evidence for imperfect frustration<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2014-05-02\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-00960280\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00960280] Incomplete devil's staircase in the magnetization curve of SrCu2(BO3)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 2014-03-17\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-00952856\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00952856] Field-induced magnetic behavior in a quasi-one-dimensional Ising-like antiferromagnet: a detailed single crystal neutron diffraction study<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2014-02-27\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:\/\/ens-lyon.hal.science\/ensl-00565060\" target=\"_blank\" rel=\"nofollow\" class=\"\">[ensl-00565060] Statics and dynamics of weakly coupled antiferromagnetic spin-1\/2 ladders 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 2011-02-10\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-00417217\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00417217] Homogeneous vs. inhomogeneous coexistence of magnetic order and superconductivity probed by NMR in Co and K doped iron pnictides<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2009-09-15\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-00398628\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00398628] Reply to the Comment by S.E. Sebastian and N. Harrison<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2009-06-24\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-00398628v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00398628] Reply to the Comment by S.E. Sebastian and N. Harrison<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2009-06-24\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-00350473v2\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00350473] Spin Configuration in the 1\/3 Magnetization Plateau of Azurite Determined by NMR<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2009-02-24\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-00340732\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00340732] Comment on \"Texture in the Superconducting Order Parameter of CeCoIn$_5$ Revealed by Nuclear Magnetic Resonance<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-11-21\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-00340732v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00340732] Comment on \"Texture in the Superconducting Order Parameter of CeCoIn$_5$ Revealed by Nuclear Magnetic Resonance<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-11-21\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-00336372\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00336372] NMR Evidence for the Persistence of a Spin Superlattice Beyond the 1\/8 Magnetization Plateau in SrCu_2(BO_3)_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 2008-11-03\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-00336372v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00336372] NMR Evidence for the Persistence of a Spin Superlattice Beyond the 1\/8 Magnetization Plateau in SrCu_2(BO_3)_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 2008-11-03\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-00274760\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00274760] Controlling Luttinger liquid physics in weakly coupled spin ladders under 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 2008-04-21\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-00271584v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00271584] Observation of a new phase transition between fully and partially polarized quantum Hall states with charge and spin gaps at $nu = 2\/3$<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-04-09\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-00271572\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00271572] NMR investigation how free are Composite Fermions at $nu = 1\/2$<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-04-09\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-00271572v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00271572] NMR investigation how free are Composite Fermions at $nu = 1\/2$<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-04-09\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-00271568\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00271568] The effects of intra-dimer Dzyaloshinsky-Moriya interaction on the properties of SrCu2(BO3)2 in an external 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 2008-04-09\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-00271568v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00271568] The effects of intra-dimer Dzyaloshinsky-Moriya interaction on the properties of SrCu2(BO3)2 in an external 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 2008-04-09\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-00270069\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00270069] Field-Induced Effects of Anisotropic Magnetic Interactions in SrCu2(BO3)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 2008-04-03\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-00268907\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00268907] Huge Transverse Magnetization in the Field-Induced Phase of the Antiferromagnetic Molecular Wheel CsFe8<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-04-01\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-00268891\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00268891] NMR Study of Large Skyrmions in Al_{0.13}Ga_{0.87}As Quantum Wells<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-04-01\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-00268891v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00268891] NMR Study of Large Skyrmions in Al_{0.13}Ga_{0.87}As Quantum Wells<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-04-01\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-00268877\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00268877] NMR evidence for the persistence of spin-superlattice above the 1\/8 magnetization plateau in SrCu2(BO3)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 2008-04-01\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-00268877v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00268877] NMR evidence for the persistence of spin-superlattice above the 1\/8 magnetization plateau in SrCu2(BO3)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 2008-04-01\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\/jpa-00247308\" target=\"_blank\" rel=\"nofollow\" class=\"\">[jpa-00247308] NMR Studies of the Normal State of 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 2008-02-04\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\/jpa-00228258\" target=\"_blank\" rel=\"nofollow\" class=\"\">[jpa-00228258] Mn N.M.R. AND MAGNETIC STRUCTURES IN (Y1-xTbx) Mn2 COMPOUNDS<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-02-04\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\/jpa-00228258v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[jpa-00228258] Mn N.M.R. AND MAGNETIC STRUCTURES IN (Y1-xTbx) Mn2 COMPOUNDS<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2008-02-04\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\/jpa-00247308v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[jpa-00247308] NMR Studies of the Normal State of 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 2008-02-04\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-00167413\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00167413] $^{77}$Se NMR evidence for the Jaccarino-Peter mechanism in the field induced superconductor, $lambda$(BETS)$_2$FeCl$_4$ }<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2007-08-20\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]<\/p>\n","protected":false},"excerpt":{"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\/gros-plan-neons-colores-abstraits-perspective-parfaits-pour-concept-scifi_181624-56907.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; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; sticky_position=&#8221;top&#8221; hover_enabled=&#8221;0&#8243; locked=&#8221;off&#8221; global_colors_info=&#8221;{}&#8221; disabled_on=&#8221;on|off|off&#8221; sticky_enabled=&#8221;0&#8243;][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; [&hellip;]<\/p>\n","protected":false},"author":12,"featured_media":10416,"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-10415","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\/10415","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=10415"}],"version-history":[{"count":0,"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/pages\/10415\/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\/10416"}],"wp:attachment":[{"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/media?parent=10415"}],"wp:term":[{"taxonomy":"folder","embeddable":true,"href":"https:\/\/lncmi.cnrs.fr\/en\/wp-json\/wp\/v2\/folder?post=10415"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}