{"id":583,"date":"2018-07-10T12:13:26","date_gmt":"2018-07-10T10:13:26","guid":{"rendered":"https:\/\/sacepe-quest.neel.cnrs.fr\/?page_id=583"},"modified":"2025-01-23T16:59:10","modified_gmt":"2025-01-23T15:59:10","slug":"highlights","status":"publish","type":"page","link":"https:\/\/sacepe-quest.neel.cnrs.fr\/index.php\/highlights\/","title":{"rendered":"Highlights"},"content":{"rendered":"<h4 class=\"c-article-title\" data-test=\"article-title\"><a href=\"https:\/\/rdcu.be\/d5puj\" target=\"_blank\" rel=\"noopener\">First-order quantum breakdown of superconductivity in an amorphous superconductor<\/a><\/h4>\n<p><img loading=\"lazy\" decoding=\"async\" class=\" wp-image-1211 alignright\" src=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2025\/01\/SIT-charpentier-211x300.png\" alt=\"\" width=\"171\" height=\"243\" srcset=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2025\/01\/SIT-charpentier-211x300.png 211w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2025\/01\/SIT-charpentier.png 627w\" sizes=\"auto, (max-width: 171px) 100vw, 171px\" \/>We discovered that highly disordered superconductors, such as indium oxide films, undergo abrupt first-order quantum phase transitions, challenging traditional theories that assume gradual transitions. Our findings, which reveal a sharp drop in superfluid stiffness at a critical disorder level, have significant implications for quantum circuits that use disordered superconductors as superinductors.&nbsp;<\/p>\n<p>T. Charpentier, D. Perconte, S. L\u00e9ger, K. Amin, F. Blondelle, F. Gay, O. Buisson, Lev I., A. Khvalyuk, I. Poboiko, M. Feigel\u2019man, N. Roch, B. Sac\u00e9p\u00e9 <a href=\"https:\/\/www.nature.com\/articles\/s41567-024-02713-8\" target=\"_blank\" rel=\"noopener\">Nature Physics (2025)<\/a><\/p>\n<p>Some news outlets: <a href=\"https:\/\/thequantuminsider.com\/2025\/01\/04\/sudden-transition-in-superconductors-could-shift-quantum-technology-into-high-gear\/\" target=\"_blank\" rel=\"noopener\">Quantum Insider<\/a>, <a href=\"https:\/\/interestingengineering.com\/science\/rare-first-order-quantum-phase-transition\" target=\"_blank\" rel=\"noopener\">Interesting Engineering<\/a>, <a href=\"https:\/\/phys.org\/news\/2025-01-quantum-phase-transition-indium-oxide.html\" target=\"_blank\" rel=\"noopener\">Phys.org<\/a>, <a href=\"https:\/\/cosmosmagazine.com\/technology\/materials\/superconductivity-quantum-phase-transition\/\" target=\"_blank\" rel=\"noopener\">Cosmos<\/a><\/p>\n<hr>\n<h4 data-test=\"article-title\">&nbsp;<\/h4>\n<h4 class=\"c-article-title\" data-test=\"article-title\"><a href=\"https:\/\/www.nature.com\/articles\/s41467-024-54211-3\" target=\"_blank\" rel=\"noopener\">Evidence for correlated electron pairs and triplets in quantum Hall interferometers<\/a><\/h4>\n<p><img loading=\"lazy\" decoding=\"async\" class=\" wp-image-1206 alignright\" src=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2025\/01\/Pairing-208x300.png\" alt=\"\" width=\"183\" height=\"264\" srcset=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2025\/01\/Pairing-208x300.png 208w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2025\/01\/Pairing.png 636w\" sizes=\"auto, (max-width: 183px) 100vw, 183px\" \/>This study we have evidenced unusual electron pairing and tripling phenomena without attractive interactions in graphene quantum Hall Fabry\u2013P\u00e9rot interferometers (QH FPIs). At a bulk filling factor of \u03bd = 2, electron pairing occurs&nbsp; while at \u03bd = 3, electron tripling emerges, characterized by a fractional Aharonov\u2013Bohm flux period of h\/2e and h\/3e, respectively. Using plunger-gate spectroscopy, we show that charge transport in this pairing and tripling regime is correlated across two and three edge channels.<\/p>\n<p>W. Yang, D. Perconte, C. D\u00e9prez, K. Watanabe, T. Taniguchi, S. Dumont, E. Wagner, F. Gay, I. Safi, H. Sellier, B. Sac\u00e9p\u00e9 <a href=\"https:\/\/www.nature.com\/articles\/s41467-024-54211-3\" target=\"_blank\" rel=\"noopener\">Nature Communications 15:10064 (2024)<\/a><\/p>\n<hr>\n<h4>&nbsp;<\/h4>\n<h4><a href=\"https:\/\/rdcu.be\/dslia\" target=\"_blank\" rel=\"noopener\">Evidence for chiral supercurrent in quantum Hall Josephson junctions<\/a><\/h4>\n<p><img loading=\"lazy\" decoding=\"async\" class=\" wp-image-1097 alignright\" src=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/12\/J33_4-2-300x297.jpg\" alt=\"\" width=\"140\" height=\"139\" srcset=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/12\/J33_4-2-300x297.jpg 300w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/12\/J33_4-2-150x150.jpg 150w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/12\/J33_4-2-768x761.jpg 768w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/12\/J33_4-2-500x500.jpg 500w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/12\/J33_4-2-230x230.jpg 230w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/12\/J33_4-2-330x330.jpg 330w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/12\/J33_4-2.jpg 826w\" sizes=\"auto, (max-width: 140px) 100vw, 140px\" \/>In this work we have tackled the complex challenge of associating two emblematic quantum phenomena of condensed matter: the quantum Hall effect and superconductivity. We demonstrated the existence of a <em>chiral Josephson supercurrent<\/em> with unprecedented properties flowing between two superconducting electrodes, connected by a graphene nanoribbon in the quantum Hall regime. This supercurrent is transported along the quantum Hall edge channels of the graphene, forming a chiral loop whose rotation direction depends on the sign of the magnetic field.<\/p>\n<p>H. Vignaud, D. Perconte, W. Yang, B. Kousar, E. Wagner, F. Gay, K. Watanabe, T. Taniguchi, H. Courtois, Z. han, H. Sellier, B. Sac\u00e9p\u00e9,<strong><a href=\"https:\/\/rdcu.be\/dslia\" target=\"_blank\" rel=\"noopener\"> Nature 624, 545 (2023)<\/a><\/strong><\/p>\n<p>&nbsp;<\/p>\n<hr>\n<h4><a href=\"https:\/\/www.science.org\/doi\/10.1126\/sciadv.adf7220\" target=\"_blank\" rel=\"noopener\">Absence of edge reconstruction for quantum Hall edge channels in graphene devices<\/a><\/h4>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-1078 alignright\" src=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/11\/edge-states2.png\" alt=\"\" width=\"138\" height=\"138\" srcset=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/11\/edge-states2.png 282w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/11\/edge-states2-150x150.png 150w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/11\/edge-states2-230x230.png 230w\" sizes=\"auto, (max-width: 138px) 100vw, 138px\" \/>This study report on the first scanning tunneling spectroscopy of quantum Hall edge channels in graphene under a perpendicular magnetic field. Our work reveals that these edge channels are confined to a few magnetic lengths at crystal edges, confirming them as ideal 1D chiral channels without&nbsp; electrostatic reconstruction. The findings carry implications for electron and heat transport experiments in graphene and other 2D crystalline materials.<\/p>\n<p>A. Coissard<span class=\"authors\"><span role=\"list\">, <span role=\"listitem\">A. G. Grushin<\/span>, <span role=\"listitem\">C. Repellin<\/span>, <span role=\"listitem\">L.Veyrat<\/span>, <span role=\"listitem\">K. Watanabe<\/span>, <span role=\"listitem\">T. Taniguchi<\/span>, <span role=\"listitem\">F. Gay<\/span>, <span role=\"listitem\">H. Courtois<\/span>, <span role=\"listitem\">H. Sellier<\/span>, <span role=\"listitem\">B. Sac\u00e9p\u00e9, <\/span><\/span><\/span><a href=\"https:\/\/www.science.org\/doi\/10.1126\/sciadv.adf7220\" target=\"_blank\" rel=\"noopener\"><strong><span class=\"ml-1\">Science Advances <\/span><span class=\"ml-1\">9, <\/span><span class=\"ml-1\">eadf7220<\/span><span class=\"ml-1\">(2023)<\/span><\/strong><\/a><\/p>\n<p>&nbsp;<\/p>\n<hr>\n<h4><a href=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2022\/05\/Coissard-Imaging-tunable-quantum-Hall-broken-symmetry-orders-in-graphene-Nature_2022.pdf\" target=\"_blank\" rel=\"noopener\">Imaging tunable quantum Hall broken-symmetry orders in graphene<\/a><\/h4>\n<p><img loading=\"lazy\" decoding=\"async\" class=\" wp-image-1007 alignright\" src=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/02\/Kekule-295x300.png\" alt=\"\" width=\"144\" height=\"147\" srcset=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/02\/Kekule-295x300.png 295w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2023\/02\/Kekule.png 395w\" sizes=\"auto, (max-width: 144px) 100vw, 144px\" \/>When electrons populate a flat band their kinetic energy becomes negligible, forcing them to organize in exotic many-body states to minimize their Coulomb energy. The zeroth Landau level of graphene under a magnetic field is a particularly interesting strongly interacting flat band because interelectron interactions are predicted to induce a rich variety of broken-symmetry states with distinct topological and lattice-scale orders, which we evidence in this work.<\/p>\n<p>A. Coissard, D. Wander, H. Vignaud, A. G. Grushin, C. Repellin, K. Watanabe, T. Taniguchi, F. Gay, C. B. Winkelmann, H. Courtois, H. Sellier, B. Sac\u00e9p\u00e9,<strong> <a href=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2022\/05\/Coissard-Imaging-tunable-quantum-Hall-broken-symmetry-orders-in-graphene-Nature_2022.pdf\" target=\"_blank\" rel=\"noopener\">Nature 605, 51 (2022)<\/a><\/strong><\/p>\n<p>&nbsp;<\/p>\n<hr>\n<h4><a href=\"https:\/\/rdcu.be\/cgw0r\" target=\"_blank\" rel=\"noopener\">A tunable Fabry-P\u00e9rot quantum Hall interferometer in graphene<\/a><\/h4>\n<p><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-950 alignright\" src=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2021\/10\/FPI-288x300.png\" alt=\"\" width=\"144\" height=\"150\" srcset=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2021\/10\/FPI-288x300.png 288w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2021\/10\/FPI.png 297w\" sizes=\"auto, (max-width: 144px) 100vw, 144px\" \/><\/p>\n<p>Electron interferometry with quantum Hall (QH) edge channels in semiconductor heterostructures can probe and harness the exchange statistics of anyonic excitations. In this work we show that high-mobility monolayer graphene constitutes an alternative material system, not affected by charging effects, for performing Fabry\u2013P\u00e9rot QH interferometry in the integer QH regime.<\/p>\n<p>C. D\u00e9prez, L. Veyrat, H. Vignaud, G. Nayak, K. Watanabe, T. Taniguchi, F. Gay, H. Sellier and B. Sac\u00e9p\u00e9, <a href=\"https:\/\/rdcu.be\/cgw0r\" target=\"_blank\" rel=\"noopener\"><strong>Nature Nanotechnology 16, 555 (2021)<\/strong><\/a><\/p>\n<hr>\n<h4><a href=\"https:\/\/rdcu.be\/b5tDq\" target=\"_blank\" rel=\"noopener noreferrer\">Review Article: Quantum breakdown of superconductivity in low-dimensional materials<\/a><\/h4>\n<p>This Review Article summarizes recent progress in understanding of the <img loading=\"lazy\" decoding=\"async\" class=\" wp-image-853 alignright\" src=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2020\/08\/2020_Focus-e1598732271718-300x217.jpg\" alt=\"\" width=\"139\" height=\"100\" srcset=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2020\/08\/2020_Focus-e1598732271718-300x217.jpg 300w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2020\/08\/2020_Focus-e1598732271718.jpg 418w\" sizes=\"auto, (max-width: 139px) 100vw, 139px\" \/>various pathways that lead to the destruction of superconductivity by the interplay of disorder, localization and interactions, including experiments in low dimensional materials and application in superconducting quantum devices.&nbsp;<\/p>\n<p>B. Sac\u00e9p\u00e9, M. Feigel&#8217;man, T. Klapwijk,<strong> <a href=\"https:\/\/rdcu.be\/b5tDq\" target=\"_blank\" rel=\"noopener noreferrer\">Nature Physics 7, 734 (2020)<\/a><\/strong><\/p>\n<hr>\n<h4><a href=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2020\/02\/Veyrat-Helical-quantum-Hall-phase-in-graphene-on-SrTiO3-Science.pdf\" target=\"_blank\" rel=\"noopener noreferrer\"><strong>Helical quantum Hall phase in graphene on SrTiO3<\/strong><\/a><\/h4>\n<p><img loading=\"lazy\" decoding=\"async\" class=\" wp-image-768 alignright\" src=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2019\/09\/graphene_edge_channels2-300x165.png\" alt=\"\" width=\"161\" height=\"89\" srcset=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2019\/09\/graphene_edge_channels2-300x165.png 300w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2019\/09\/graphene_edge_channels2-768x422.png 768w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2019\/09\/graphene_edge_channels2-1024x563.png 1024w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2019\/09\/graphene_edge_channels2.png 2000w\" sizes=\"auto, (max-width: 161px) 100vw, 161px\" \/>We unveiled a new interaction-induced topological phase in the zeroth Landau level of graphene. This phase is insulating in the bulk and exhibits a pair of spin-filtered, helical edge channels. It emerges under moderate perpendicular magnetic field when graphene is placed in proximity to a high-k dielectric substrate. In this work we demonstrated a remarkably robust quantum spin Hall effect that withstands up to 110 K over micron-long distances which opens a new avenue for spintronics and topological superconductivity.<\/p>\n<p>L. Veyrat, C. Deprez, A. Coissard, X. Li, F. Gay, K. Watanabe, T. Taniguchi, Vitto Han, B. Piot, H. Sellier, B. Sac\u00e9p\u00e9, <strong><a href=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2020\/02\/Veyrat-Helical-quantum-Hall-phase-in-graphene-on-SrTiO3-Science.pdf\" target=\"_blank\" rel=\"noopener noreferrer\">Science 367, 781 (2020)<\/a><\/strong><\/p>\n<hr>\n<h4><a href=\"https:\/\/rdcu.be\/bfLit\"><strong>When Joule poisons Majorana in topological Josephson junctions<\/strong><img loading=\"lazy\" decoding=\"async\" class=\" wp-image-694 alignright\" src=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2019\/01\/Shapiro-e1546944898676-297x300.png\" alt=\"\" width=\"127\" height=\"128\" srcset=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2019\/01\/Shapiro-e1546944898676-297x300.png 297w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2019\/01\/Shapiro-e1546944898676-150x150.png 150w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2019\/01\/Shapiro-e1546944898676-230x230.png 230w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2019\/01\/Shapiro-e1546944898676-330x330.png 330w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2019\/01\/Shapiro-e1546944898676.png 353w\" sizes=\"auto, (max-width: 127px) 100vw, 127px\" \/><\/a><\/h4>\n<p>The search for experimental evidence of Majorana modes is an area of intense research in condensed matter and quantum physics and uncovering clear evidence is complicated. We investigate the impact of Joule heating which can influence the analysis of experimental features related to Majorana bound states in topological Josephson junctions.<\/p>\n<p>K. Le Calvez, L. Veyrat, F. Gay, P. Plaindoux, C. Winkelmann, H. Courtois, B. Sac\u00e9p\u00e9,&nbsp;<a href=\"https:\/\/rdcu.be\/bfLit\" target=\"_blank\" rel=\"noopener noreferrer\"><strong>Communications Physics<\/strong> 2:4 (2019)<\/a><\/p>\n<hr>\n<h4><a href=\"https:\/\/www.nature.com\/articles\/s41567-018-0294-6\" target=\"_blank\" rel=\"noopener noreferrer\"><strong>Low-temperature anomaly in disordered superconductors near <span id=\"MathJax-Element-1-Frame\" class=\"MathJax\" tabindex=\"0\"><span id=\"MathJax-Span-1\" class=\"math\"><span id=\"MathJax-Span-2\" class=\"mrow\"><span id=\"MathJax-Span-3\" class=\"msubsup\"><span id=\"MathJax-Span-4\" class=\"mi\">B<\/span><span id=\"MathJax-Span-5\" class=\"texatom\"><span id=\"MathJax-Span-6\" class=\"mrow\"><span id=\"MathJax-Span-7\" class=\"mi\">c<\/span><\/span><\/span><\/span><\/span><\/span><\/span><\/strong><strong><span id=\"MathJax-Element-1-Frame\" class=\"MathJax\" tabindex=\"0\"><span id=\"MathJax-Span-1\" class=\"math\"><span id=\"MathJax-Span-2\" class=\"mrow\"><span id=\"MathJax-Span-3\" class=\"msubsup\"><span id=\"MathJax-Span-5\" class=\"texatom\"><span id=\"MathJax-Span-6\" class=\"mrow\"><span id=\"MathJax-Span-8\" class=\"mn\">2 as a vortex-glass property<\/span><\/span><\/span><\/span><\/span><\/span><\/span><\/strong><\/a><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-624 alignright\" src=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/10\/Phasediagram-4-1-202x300.png\" alt=\"\" width=\"145\" height=\"215\" srcset=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/10\/Phasediagram-4-1-202x300.png 202w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/10\/Phasediagram-4-1-768x1142.png 768w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/10\/Phasediagram-4-1-688x1024.png 688w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/10\/Phasediagram-4-1.png 1635w\" sizes=\"auto, (max-width: 145px) 100vw, 145px\" \/><span id=\"MathJax-Element-1-Frame\" class=\"MathJax\" tabindex=\"0\"><span id=\"MathJax-Span-1\" class=\"math\"><span id=\"MathJax-Span-2\" class=\"mrow\"><span id=\"MathJax-Span-3\" class=\"msubsup\"><span id=\"MathJax-Span-5\" class=\"texatom\"><span id=\"MathJax-Span-6\" class=\"mrow\"><span id=\"MathJax-Span-8\" class=\"mn\"><\/span><\/span><\/span><\/span><\/span><\/span><\/span><\/h4>\n<div class=\"t m0 x2 hf y7c ffb fsc fc1 sc0 ls0 ws42\"><span class=\"current-selection\">Strongly disor<\/span><span class=\"current-selection\">dered super<\/span><span class=\"current-selection\">c<\/span><span class=\"current-selection\">onductors in a magnetic field e<\/span><span class=\"current-selection\">xhibit many char<\/span><span class=\"current-selection\">acteristic properties of type-II super<\/span><span class=\"current-selection\">conductivit<\/span><span class=\"current-selection\">y<\/span><span class=\"current-selection\">\u2014<\/span><span class=\"current-selection\">ex<\/span><span class=\"current-selection\">cept at lo<\/span><span class=\"current-selection\">w temper<\/span><span class=\"current-selection\">atur<\/span><span class=\"current-selection\">es, where an anomalous linear t<\/span><span class=\"current-selection\">emper<\/span><span class=\"current-selection\">ature <\/span><span class=\"current-selection\">dependenc<\/span><span class=\"current-selection\">e of the r<\/span><span class=\"current-selection\">esistiv<\/span><span class=\"current-selection\">e critical field B<\/span><span class=\"current-selection\">c2<\/span><span class=\"current-selection\"> is routinely <\/span><span class=\"current-selection\">observ<\/span><span class=\"current-selection\"><span class=\"current-selection\">ed. Here we<\/span><\/span><span class=\"current-selection\"> r<\/span><span class=\"current-selection\">eport sy<\/span><span class=\"current-selection\">stematic measur<\/span><span class=\"current-selection\">ements of the critical magnetic field and current on amorphous indium o<\/span><span class=\"current-selection\">xide films which <\/span><span class=\"current-selection\">show that the B<\/span><span class=\"current-selection\">c2 <\/span><span class=\"current-selection\">anomaly is acc<\/span><span class=\"current-selection\">ompanied by mean-<\/span><span class=\"current-selection\">field-lik<\/span><span class=\"current-selection\">e scaling of <\/span><span class=\"current-selection\">the critical current. Based on a c<\/span><span class=\"current-selection\">omprehensiv<\/span><span class=\"current-selection\">e theoretical study w<\/span><span class=\"current-selection\">e demonstrate that these observ<\/span><span class=\"current-selection\">ations are a c<\/span><span class=\"current-selection\">onsequenc<\/span><span class=\"current-selection\">e of the <\/span><span class=\"current-selection\">v<\/span><span class=\"current-selection\">ortex<\/span><span class=\"current-selection\">-glass gr<\/span><span class=\"current-selection\">ound state and its thermal fluctuations.<\/span><\/div>\n<div>&nbsp;<\/div>\n<div>&nbsp;B. Sac\u00e9p\u00e9, J. Seidemann, F. Gay, K. Davenport, A. Rogachev, M. Ovadia, K. Michaeli, M. V. Feigel&#8217;man <a href=\"https:\/\/rdcu.be\/8MQu\" target=\"_blank\" rel=\"noopener noreferrer\"><em><strong>Nature Physics<\/strong><\/em> 15, 48-53 (2019)<\/a>&nbsp;<\/div>\n<div><em>&nbsp;See also CNRS press release<\/em> : <a href=\"http:\/\/www.cnrs.fr\/inp\/spip.php?article6274\" target=\"_blank\" rel=\"noopener noreferrer\">http:\/\/www.cnrs.fr\/inp\/spip.php?article6274<\/a><\/div>\n<div>&nbsp;<\/div>\n<hr>\n<h4 class=\"tighten-line-height small-space-below\" data-test=\"article-title\"><a href=\"https:\/\/www.nature.com\/articles\/s41567-018-0179-8\" target=\"_blank\" rel=\"noopener noreferrer\"><strong>Pair-breaking quantum phase transition in superconducting nanowires<\/strong><img loading=\"lazy\" decoding=\"async\" class=\"wp-image-575 alignright\" src=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/07\/pairbreaking_v4-300x225.jpg\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" srcset=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/07\/pairbreaking_v4-300x225.jpg 300w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/07\/pairbreaking_v4-768x576.jpg 768w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/07\/pairbreaking_v4-1024x768.jpg 1024w\" alt=\"\" width=\"225\" height=\"169\"><\/a><\/h4>\n<p>Transport measurements performed on MoGe superconducting nanowires reveal a quantitative agreement with quantum critical behaviour driven by a pair-breaking mechanism.<\/p>\n<p class=\"text14 standard-space-below\">Hyunjeong Kim, Fr\u00e9d\u00e9ric Gay, Adrian Del Maestro, Benjamin Sac\u00e9p\u00e9, Andrey Rogachev. <a href=\"https:\/\/www.nature.com\/articles\/s41567-018-0179-8\" target=\"_blank\" rel=\"noopener noreferrer\"><i data-test=\"journal-title\"><strong>Nature Physics<\/strong><\/i> (<span data-test=\"article-publication-year\">2018)<\/span><\/a><\/p>\n<p>&nbsp;<\/p>\n<p>&nbsp;<\/p>\n<hr>\n<h4><a href=\"https:\/\/www.nature.com\/articles\/ncomms14983\" target=\"_blank\" rel=\"noopener noreferrer\"><strong>Pinching off electron edge-channels in graphene<\/strong><img loading=\"lazy\" decoding=\"async\" class=\"size-medium wp-image-590 alignright\" src=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/07\/Graphene-QPC-300x169.jpg\" alt=\"\" width=\"300\" height=\"169\" srcset=\"https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/07\/Graphene-QPC-300x169.jpg 300w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/07\/Graphene-QPC-768x432.jpg 768w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/07\/Graphene-QPC-1024x576.jpg 1024w, https:\/\/sacepe-quest.neel.cnrs.fr\/wp-content\/uploads\/2018\/07\/Graphene-QPC.jpg 1920w\" sizes=\"auto, (max-width: 300px) 100vw, 300px\" \/><\/a><\/h4>\n<p>High mobility graphene van der Waals heterostructures equipped with split-gate electrodes enable to control the transmission of integer and fractional quantum Hall edge channels in a gate tunable fashion, demonstrating Quantum Point Contact operation in the quantum Hall regime of graphene.<\/p>\n<p>Anna Jordan<span class=\"js-separator\">, <\/span>Fr\u00e9d\u00e9ric Gay<span class=\"js-separator\">, <\/span>Kenji Watanabe<span class=\"js-separator\">, <\/span>Takashi Taniguchi<span class=\"js-separator\">, <\/span>Zheng Han,&nbsp;Vincent Bouchiat,&nbsp;Hermann Sellier<span class=\"js-separator js-mq480-hide\">, <\/span>Benjamin Sac\u00e9p\u00e9, <a href=\"https:\/\/www.nature.com\/articles\/ncomms14983\" target=\"_blank\" rel=\"noopener noreferrer\"><strong><em>Nature Communications<\/em><\/strong> 8:14983 (2017)<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"<p>First-order quantum breakdown of superconductivity in an amorphous superconductor We discovered that highly disordered superconductors, such as indium oxide films, undergo abrupt first-order quantum phase transitions, challenging traditional theories that assume gradual transitions. Our findings, which reveal a sharp drop<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":0,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"ngg_post_thumbnail":0,"footnotes":""},"class_list":["post-583","page","type-page","status-publish","hentry"],"_links":{"self":[{"href":"https:\/\/sacepe-quest.neel.cnrs.fr\/index.php\/wp-json\/wp\/v2\/pages\/583","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/sacepe-quest.neel.cnrs.fr\/index.php\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/sacepe-quest.neel.cnrs.fr\/index.php\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/sacepe-quest.neel.cnrs.fr\/index.php\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/sacepe-quest.neel.cnrs.fr\/index.php\/wp-json\/wp\/v2\/comments?post=583"}],"version-history":[{"count":37,"href":"https:\/\/sacepe-quest.neel.cnrs.fr\/index.php\/wp-json\/wp\/v2\/pages\/583\/revisions"}],"predecessor-version":[{"id":1225,"href":"https:\/\/sacepe-quest.neel.cnrs.fr\/index.php\/wp-json\/wp\/v2\/pages\/583\/revisions\/1225"}],"wp:attachment":[{"href":"https:\/\/sacepe-quest.neel.cnrs.fr\/index.php\/wp-json\/wp\/v2\/media?parent=583"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}