{"id":11287,"date":"2024-09-10T15:40:54","date_gmt":"2024-09-10T13:40:54","guid":{"rendered":"https:\/\/lncmi.cnrs.fr\/?page_id=11287"},"modified":"2025-06-13T14:40:50","modified_gmt":"2025-06-13T12:40:50","slug":"paramagnetic-relaxation-enhancement","status":"publish","type":"page","link":"https:\/\/lncmi.cnrs.fr\/en\/optics-and-diluted-matter\/paramagnetic-relaxation-enhancement\/","title":{"rendered":"Paramagnetic relaxation enhancement"},"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;Paramagnetic relaxation enhancement&#8221; text_orientation=&#8221;center&#8221; background_overlay_color=&#8221;rgba(0,0,0,0.2)&#8221; _builder_version=&#8221;4.27.0&#8243; _module_preset=&#8221;default&#8221; background_image=&#8221;https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2024\/09\/dynamic-light-painting-background.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|off|off&#8221; _builder_version=&#8221;4.26.0&#8243; _module_preset=&#8221;default&#8221; overflow-x=&#8221;auto&#8221; sticky_position=&#8221;top&#8221; overflow-x_tablet=&#8221;auto&#8221; overflow-x_phone=&#8221;auto&#8221; overflow-x_last_edited=&#8221;on|phone&#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; _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; module_id=&#8221;description&#8221; _builder_version=&#8221;4.27.2&#8243; _module_preset=&#8221;default&#8221; locked=&#8221;off&#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_image src=&#8221;https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2025\/03\/PRE_01f-3.png&#8221; title_text=&#8221;PRE_01f&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; custom_padding=&#8221;|340px||340px||&#8221; global_colors_info=&#8221;{}&#8221;][\/et_pb_image][\/et_pb_column][\/et_pb_row][et_pb_row _builder_version=&#8221;4.25.2&#8243; _module_preset=&#8221;default&#8221; custom_padding=&#8221;|0px||||&#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; width=&#8221;100%&#8221; custom_margin=&#8221;|-309px||||&#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>In nuclear magnetic resonance (NMR), magnetic field dependent phenomena attract considerable interest: <strong>Paramagnetic relaxation enhancement<\/strong> (PRE) of NMR relaxivities induced by paramagnetic relaxation agents is theoretically, experimentally and from the application point of view a growing research area.<\/p>\n<p><span class=\"fontstyle0\">PRE is generated by the fluctuating hyperfine interaction between the magnetic moment of the <\/span><span class=\"fontstyle0\">paramagnetic compound in solution and the nuclear spin of the environment, often protons <\/span><span class=\"fontstyle0\">of water. This process enhances the longitudinal <\/span><span class=\"fontstyle0\">and transverse <\/span><span class=\"fontstyle0\">nuclear spin relaxation rates.<\/span><\/p>\n<p>The burning question here concerns the development of effective and efficient relaxation agents which can be discovered through an improved understanding of PRE mechanisms. PRE plays an increasingly important role in technical magnetic resonance imaging (MRI) for process engineering and material science. There, the image contrast quality can be significantly enhanced through application of an appropriate contrast agent for exploration of the question and sample under investigation.<\/p>\n<p>Moreover, technical MRI tends to use very high magnetic fields with 28.2 T (1200 MHz) commercially available. Since conventional relaxation agents have been tailored for much smaller magnetic fields and actually <em>decrease<\/em> in efficiency above 4.7 T (200 MHz), there is a need to develop new relaxation agents for the high magnetic field applications which are now available.<\/p>\n<p><strong>The PRE activity at LNCMI Grenoble responds to this need and allows PRE studies up to 1.4 GHz\/33 T using resistive magnets. It also includes the development of tailored NMR hardware and methods.<\/strong><\/p>\n<p>The activity benefits from a strong collaboration with research teams at the Karlsruhe Institute of Technology (KIT) in Germany.<\/p>\n<\/div>\n<p>[\/et_pb_text][\/et_pb_column][\/et_pb_row][\/et_pb_section][et_pb_section fb_built=&#8221;1&#8243; 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;4.27.0&#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-11285' id='rt-team-container-1249810942'  data-layout='layout2' data-desktop-col='2'  data-tab-col='2'  data-mobile-col='1' data-sc-id='11285' 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=\"17727\"><div class=\"single-team-area\"><div class=\"img-area rt-col-sm-2 rt-col-xs-4 \"><figure><a class=\"\" data-id=\"17727\" target=\"_self\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/kramer-steffen\/\"><img loading=\"lazy\" decoding=\"async\" width=\"300\" height=\"300\" src=\"https:\/\/lncmi.cnrs.fr\/wp-content\/uploads\/2024\/09\/Steffen_KRAMER.jpg\" class=\"img-responsive rt-team-img\" alt=\"KR\u00c4MER Steffen\" \/><\/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=\"17727\" target=\"_self\" title=\"KR\u00c4MER Steffen\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/kramer-steffen\/\">KR\u00c4MER Steffen<\/a><\/span><\/h3><div class=\"tlp-position\"><a class=\"\" data-id=\"17727\" target=\"_self\" title=\"KR\u00c4MER Steffen\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/kramer-steffen\/\">Paramagnetic relaxation enhancement, Scientific Instrumentation<\/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 class=\"readmore-btn\"><\/div><div class=\"readmore-btn hirme-resume\"><a class=\"rt-ream-me-btn\" data-id=\"17727\" target=\"_self\" title=\"KR\u00c4MER Steffen\" href=\"https:\/\/lncmi.cnrs.fr\/en\/annuaire\/kramer-steffen\/\">Read More<\/a><\/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; 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; locked=&#8221;off&#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 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; width=&#8221;74.1%&#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\/03\/PRE02.png&#8221; title_text=&#8221;PRE02&#8243; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; width=&#8221;100%&#8221; custom_padding=&#8221;|||0px||&#8221; global_colors_info=&#8221;{}&#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; width=&#8221;70.2%&#8221; custom_margin=&#8221;|||211px||&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<h3><strong>PRE studies on lanthanide compounds<\/strong><\/h3>\n<p>Aequeous solutions of molecular compounds containing lanthanide ions with a total spin J&gt;0 are known to exhibit intersting PRE properties up to highest magnetic fields. The short electronic correlation times of the lanthanide ions can cause a strong increase of the PRE with magnetic field due to a Curie spin contribution, i.e., the time averaged magnetic moment of the lanthanide.<\/p>\n<p>PRE studies of such compounds up to highest magnetic fields are important not only for the theoretical description and understanding of the interaction of the compounds with the solvent, but also with respect to their applications in MRI.<\/p>\n<p><span class=\"HwtZe\" lang=\"en\"><span class=\"jCAhz ChMk0b\"><span class=\"ryNqvb\">Since 2014, LNCMI has been conducting systematic high-field PRE studies on inorganic paramagnetic complexes containing lanthanide ions.<\/span><\/span><\/span><\/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; custom_margin=&#8221;|731px||auto||&#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\/03\/Fig_Hom.png&#8221; title_text=&#8221;Fig_Hom&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; width=&#8221;476px&#8221; height=&#8221;300px&#8221; custom_margin=&#8221;|7px||||&#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; width=&#8221;71.2%&#8221; custom_margin=&#8221;|||211px||&#8221; custom_padding=&#8221;|0px||0px||false&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<h3><strong>NMR hardware and methods development<\/strong><\/h3>\n<p><span class=\"fontstyle0\">Most proton <\/span><span class=\"fontstyle0\">PRE studies end up at frequencies below 800 MHz\/18.8 T. <\/span><span class=\"fontstyle0\">However, recent progress in superconducting magnets has opened the way for a new generation of very homogeneous and stable high-field magnets. Nowadays, commercial high-resolution NMR magnets operate up to 1200 MHz\/28.2 T<\/span><span class=\"fontstyle0\">. <\/span><\/p>\n<p>Despite this progress, the high-power, water-cooled resistive magnets of facilities dedicated to intense magnetic fields, such as the LNCMI in Grenoble, still exceed these field strengths and enable PRE studies at even more intense magnetic fields.<\/p>\n<p>However, NMR experiments in resistive high field magnets are hampered by their intrinsically low field homogeneity and field stability, as well as by a limited access time and high running costs.<\/p>\n<p>In order to overcome these limitions, we constantly develop tailored NMR instruments (broadband tunable NMR probes, microliter sample volumes) and methods (single scan NMR, deconvolution techniques, saturation recovery and CPMG sequences) for PRE studies up to highest possible fields.<\/p>\n<p>[\/et_pb_text][\/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;4.27.4&#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;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<h3 class=\"entry-title\">Experimental technique<\/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;Nuclear Magnetic Resonance&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;][\/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;4.27.0&#8243; _module_preset=&#8221;default&#8221; locked=&#8221;off&#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>Selected publications<\/h3>\n<p>&nbsp;<\/p>\n<h4><strong>PRE studies of lanthanide compounds<\/strong><\/h4>\n<ul>\n<li>N. Schork et al., NMR Relaxivities of Paramagnetic, Ultra-High Spin Heterometallic Clusters within Polyoxometalate Matrix as a Function of Solvent and Metal Ion, <a href=\"https:\/\/doi.org\/10.1002\/cphc.202200215\" target=\"_blank\" rel=\"noopener\"><i>ChemPhysChem<\/i> <b>2022<\/b>, <i>23<\/i>, e202200215<\/a><\/li>\n<li>A. C. Venu <em>et al.<\/em>, NMR Relaxivities of Paramagnetic Lanthanide-Containing Polyoxometalates, <a href=\"https:\/\/doi.org\/10.3390\/molecules26247481\" target=\"_blank\" rel=\"noopener\"><em>Molecules<\/em> <b>2021<\/b>, <em>26<\/em>(24), 7481<\/a><\/li>\n<li>M. Ibrahim <em>et al.<\/em>,Polyoxometalate-based high-spin cluster systems: a NMR relaxivity study up to 1.4 GHz\/33 T,\u00a0 <a href=\"https:\/\/doi.org\/10.1039\/C9DT02052G\" target=\"_blank\" rel=\"noopener\"><i>Dalton Transactions<\/i> <strong>2019, <\/strong>48.41, 15597-15604<\/a><\/li>\n<li>G. Guthausen <em>et al.<\/em>,Characterisation and application of ultra-high spin clusters as magnetic resonance relaxation agents, <a href=\"https:\/\/doi.org\/10.1039\/C4DT02916J\" target=\"_blank\" rel=\"noopener\"><i>Dalton Transactions<\/i> <strong>2015 <\/strong>44.11, 5032-5040<\/a><\/li>\n<\/ul>\n<h4><strong>Development of NMR hardware and methods for PRE in high magnetic fields<\/strong><\/h4>\n<ul>\n<li>R. Nasser Din <em>et al.<\/em>, Longitudinal and Transverse <sup>1<\/sup>H Nuclear Magnetic Resonance Relaxivities of Lanthanide Ions in Aqueous Solution up to 1.4 GHz\/33 T, <a href=\"https:\/\/doi.org\/10.3390\/molecules29204956\" target=\"_blank\" rel=\"noopener\"><em>Molecules<\/em> <b>2024<\/b>, <em>29<\/em>(20), 4956<\/a><\/li>\n<li>R. Nasser Din, Nuclear magnetic resonance studies of paramagnetic relaxation enhancement at high magnetic fields : methods and applications, <a href=\"https:\/\/theses.hal.science\/tel-04578182v1\" target=\"_blank\" rel=\"noopener\">PhD thesis, Universit\u00e9 Grenoble Alpes, 2024<\/a><\/li>\n<\/ul>\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;HAL PUBLICATIONS&#8221; _builder_version=&#8221;4.27.4&#8243; _module_preset=&#8221;default&#8221; global_colors_info=&#8221;{}&#8221;]<\/p>\n<p><span style=\"color: #3c434a;font-family: Consolas, Monaco, monospace;font-size: 11.7px;font-style: normal;font-weight: 400;letter-spacing: normal;text-align: start;text-indent: 0px;text-transform: none;float: none\"><div class=\"wp-rss-template-container\" data-wpra-template=\"default\" data-template-ctx=\"eyJzb3VyY2VzIjoiMTEyNzgifQ==\">\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-05210464v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-05210464] Spin-Stripe Order Tied to the Pseudogap Phase in La 1.8 \u2212 x Eu 0.2 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 2025-08-14\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-04950854v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04950854] Hysteresis and Kinetics of the First-Order Phase Transition: Losses in Magnetocaloric Effect Illustrated on the Ni-Mn-Ga-Cu<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2025-02-17\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-04945301v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04945301] Signatures of two gaps in the spin susceptibility 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 2025-02-13\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-04830512v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04830512] Magnetic Fields and Measurements<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2024-12-11\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-04830502v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04830502] Comparative NMR Relaxivity Study of Polyoxometalate-Based Clusters [Mn4(H2O)2(P2W1SO56)2]16\u2212 and [{Dy(H2O)6}2Mn4(H2O)2(P2W15O56)2]10\u2212 from 20\u00a0MHz to 1.2\u00a0GHz<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2024-12-11\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-04830494v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04830494] Polyoxometalate-based high-spin cluster systems: a NMR relaxivity study up to 1.4 GHz\/33 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 2024-12-11\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-04765445v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04765445] Helium pool boiling critical heat flux under various magnetically controlled gravity levels<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2024-11-04\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-04765434v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04765434] Influence of multiaxial isothermal forging on magnetocaloric effect and magnetostructural transition in Ni-Mn-Ga-Si alloy<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2024-11-04\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-04765409v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04765409] NMR Relaxivities of Paramagnetic, Ultra\u2010High Spin Heterometallic Clusters within Polyoxometalate Matrix as a Function of Solvent and Metal Ion<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2024-11-04\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-04765388v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04765388] NMR Relaxivities of Paramagnetic Lanthanide-Containing Polyoxometalates<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2024-11-04\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-04294982v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-04294982] 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 2023-11-20\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.insa-toulouse.fr\/hal-03871930\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03871930] Energy Efficiency of Resistive High Field Magnets: Aspects of Magnet Technology, Power Supply Operation and Field Quality<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2022-11-25\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:\/\/insa-toulouse.hal.science\/hal-03871930v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03871930] Energy Efficiency of Resistive High Field Magnets: Aspects of Magnet Technology, Power Supply Operation and Field Quality<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2022-11-25\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-03787195v1\" 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-03679816\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03679816] Competing magnetic phases in the frustrated spin-1\/2 chain compound \u03b2\u2212TeVO4 probed 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 2022-05-27\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-03679816v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03679816] Competing magnetic phases in the frustrated spin-1\/2 chain compound \u03b2\u2212TeVO4 probed 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 2022-05-27\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-03440900\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03440900] Tunneling spectroscopy of few-monolayer NbSe$_2$ in high magnetic field: Ising protection and triplet superconductivity<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2021-11-22\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-03440900v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03440900] Tunneling spectroscopy of few-monolayer NbSe$_2$ in high magnetic field: Ising protection and triplet superconductivity<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2021-11-22\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-03060546v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-03060546] High magnetic field ultrasound study of spin freezing in La$_{1.88}$Sr$_{0.12}$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 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-02576102v1\" 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-03024412v1\" 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-02936114\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02936114] Presaturation phase in the frustrated ferro-antiferromagnet Pb2VO(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 2020-11-18\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-02936114v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02936114] Presaturation phase in the frustrated ferro-antiferromagnet Pb2VO(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 2020-11-18\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-02936756\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02936756] Thermal effects versus spin nematicity in a frustrated spin-1\/2 chain<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2020-09-11\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-02936756v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-02936756] Thermal effects versus spin nematicity in a frustrated spin-1\/2 chain<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2020-09-11\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-02305943v1\" 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-01998113v1\" 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-01998175\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01998175] Dichotomy between Attractive and Repulsive Tomonaga-Luttinger Liquids in Spin Ladders<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-05-29\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-01998175v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01998175] Dichotomy between Attractive and Repulsive Tomonaga-Luttinger Liquids in Spin Ladders<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2019-05-29\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-01992211\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992211] Critical Doping for the Onset of a Two-Band Superconducting Ground State in SrTiO 3 \u2212 \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 2019-05-29\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-01992211v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992211] Critical Doping for the Onset of a Two-Band Superconducting Ground State in SrTiO 3 \u2212 \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 2019-05-29\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-01998565v1\" 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-01998228\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01998228] Spin dynamics in the high-field phases of 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-01998228v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01998228] Spin dynamics in the high-field phases of 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-01998084v1\" 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-01997584v1\" 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-01992535v1\" 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-01992484\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992484] Spin susceptibility of charge-ordered YBa 2 Cu 3 O y across the upper critical 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 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-01992484v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992484] Spin susceptibility of charge-ordered YBa 2 Cu 3 O y across the upper critical 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 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-01992207v1\" 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-01992184\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992184] A loop-gap resonator for chirality-sensitive nuclear magneto-electric resonance (NMER)<\/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-01992184v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992184] A loop-gap resonator for chirality-sensitive nuclear magneto-electric resonance (NMER)<\/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-01992177\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992177] Characterisation and application of ultra-high spin clusters as magnetic resonance relaxation agents<\/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-01992177v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992177] Characterisation and application of ultra-high spin clusters as magnetic resonance relaxation agents<\/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-01992173\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992173] Nuclear Magnetic Resonance Relaxivities: Investigations of Ultrahigh-Spin Lanthanide Clusters from 10 MHz to 1.4 GHz<\/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-01992173v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01992173] Nuclear Magnetic Resonance Relaxivities: Investigations of Ultrahigh-Spin Lanthanide Clusters from 10 MHz to 1.4 GHz<\/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-01681751\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01681751] Nuclear magnetic resonance in high magnetic field: Application to condensed matter 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 2018-01-11\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-01681751v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-01681751] Nuclear magnetic resonance in high magnetic field: Application to condensed matter 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 2018-01-11\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-00986315v1\" 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-00960280v1\" 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-00844437\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00844437] Microscopic properties of the \"pinwheel\" kagome compound Rb2Cu3SnF12<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2013-07-15\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-00844437v1\" target=\"_blank\" rel=\"nofollow\" class=\"\">[hal-00844437] Microscopic properties of the \"pinwheel\" kagome compound Rb2Cu3SnF12<\/a>\n\n\n\n\n\n\n<div class=\"wprss-feed-meta\">\n    \n            <span class=\"feed-date\">\n            Published on Hal on 2013-07-15\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-00268907v1\" 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        <\/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; 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