Réunion thématique "SUpraconductivité du GDR MEETICC

›9:00 (15min)

Welcome - Information

› Amphi Buffon

9:00 - 9:15 (15min)

Welcome - Information

Amphi Buffon

›9:15 (1h30)

Cuprates
Alain Sacuto

› Amphi Buffon

9:15 - 10:45 (1h30)

Cuprates

Amphi Buffon

Alain Sacuto

› Evidence for coexistence of charge and antiferromagnetic orders in a high Tc superconductor - Cyril Proust, Laboratoire national des champs magnétiques intenses, CNRS, Toulouse 09:15-09:45 (30min)

› Distinguishing electronic anisotropy from nematic correlation in the cuprates - Indranil Paul, Laboratoire Matériaux et Phénomènes Quantiques, Univ. Paris, CNRS 09:45-10:15 (30min)

› Loop currents in high-temperature superconductors - Philippe Bourges, Laboratoire Léon Brillouin, CEA Saclay 10:15-10:45 (30min)

›10:45 (30min)

Coffee break

› Amphi Buffon

10:45 - 11:15 (30min)

Coffee break

Amphi Buffon

›11:15 (3h15)

New approaches and techniques
Yann Gallais

› Amphi Buffon

11:15 - 14:30 (3h15)

New approaches and techniques

Amphi Buffon

Yann Gallais

› Manipulating matter by strong coupling to the vacuum field - Thomas Ebbesen, Université de Strasbourg 11:15-11:45 (30min)

› Diamond-based quantum sensing for high-pressure superconductivity - Jean-François Roch, LuMIn, ENS Paris Saclay 11:45-12:15 (30min)

›12:15 (1h45)

Lunch

› Amphi Buffon

12:15 - 14:00 (1h45)

Lunch

Amphi Buffon

›14:00 (30min)

New approaches and techniques
Yann Gallais

› Amphi Buffon

14:00 - 14:30 (30min)

New approaches and techniques

Amphi Buffon

Yann Gallais

› Exploring THz electrodynamics of superconductors with Kinetic Inductance Detectors - Florence Levy-Bertrand, Institut Néel, CNRS 14:00-14:30 (30min)

›14:30 (1h40)

New SC materials
Dorothée Colson

› Amphi Buffon

14:30 - 16:10 (1h40)

New SC materials

Amphi Buffon

Dorothée Colson

› Nickelate superconductors - Andrés Cano, Institut Néél, CNRS - Baptiste Vignolle, Institut de Chimie de la Matière Condensée de Bordeaux, CNRS, Univ. Bordeaux 14:30-15:10 (40min)

› New As/Se-free iron-based superconductors by topotactic fluorination of intermetallics - Sophie Tencé, CNRS, Université de Bordeaux, ICMCB 15:30-15:50 (20min)

› Optical Identification of the Superconductive Band Gap in Nickelate Nd0.8Sr0.2NiO2 - Rebecca Cervasio, AILES/Synchrotron SOLEIL 15:30-15:50 (20min)

› Universal magnetic phase in Fe based 1D superconductors : a requirement for superconductivity ? - Victor Balédent, Laboratoire de Physique des Solides, Univ. Paris Saclay 15:50-16:10 (20min)

›16:10 (30min)

Coffee break

› Amphi Buffon

16:10 - 16:40 (30min)

Coffee break

Amphi Buffon

›16:40 (1h)

Sr2RuO4
Indranil Paul

› Amphi Buffon

16:40 - 17:40 (1h)

Sr2RuO4

Amphi Buffon

Indranil Paul

› Is the pairing in Sr2RuO4 inter-orbital? - Clifford Hicks, University of Birmingham, Max Planck Institute Dresden 16:40-17:10 (30min)

› Towards an understanding of the pairing state of Sr2RuO4 - Antoine Georges, Collège de France, Flatiron Institute 17:10-17:40 (30min)

›17:40 (2h50)

Cocktail Poster session

› Amphi Buffon

17:40 - 20:30 (2h50)

Cocktail Poster session

Amphi Buffon

›17:40 (2h50)

Poster

17:40 - 20:30 (2h50)

Poster

› A novel view of superconductivity - 17:40-20:30 (2h50)

› Absence of superconductivity in bulk layered doped Ni1+ nickelates - 17:40-20:30 (2h50)

› Accurate modeling of FeSe with screened Fock exchange and Hund's metal correlations - 17:40-20:30 (2h50)

› All-oxide High-Temperature Superconducting Spin-Valve - 17:40-20:30 (2h50)

› BCS superconductivity under a Berry curvature: when topology affects correlated phases - 17:40-20:30 (2h50)

› Doping-driven pseudogap-metal-to-metal transition in correlated electron systems - 17:40-20:30 (2h50)

› Electronics excitations in cuprates superconductors explored by Raman scattering - 17:40-20:30 (2h50)

› Evidence for coexistence of charge and antiferromagnetic orders in a high Tc superconductor - 17:40-20:30 (2h50)

› Extremely long-range Josephson coupling across a half metallic ferromagnet in proximity with a cuprate - 17:40-20:30 (2h50)

› Half-filled planes of 4ax4a interacting bipolarons: a key for understanding high Tc superconductivity - 17:40-20:30 (2h50)

› High pressure study of UTe2 in pulsed magnetic field - 17:40-20:30 (2h50)

› High sensitivity measurement of the oxygen stoichiometry of a superconducting oxide by SIMS - 17:40-20:30 (2h50)

› High-Tc superconductivity in strongly overdoped cuprates - 17:40-20:30 (2h50)

› Infinite-layer nickelate: Charge or magnetic excitation in function of the capping layer presence - 17:40-20:30 (2h50)

› Laser doped Si:B – From the material to superconducting nano-devices - 17:40-20:30 (2h50)

› Magnetic quantum phase transition at the pseudogap boundary in La1.8-xEu0.2SrxCuO4 in high fields - 17:40-20:30 (2h50)

› On-chip Spectrometers operating at 90GHz - 17:40-20:30 (2h50)

› Orbital dichotomy of Fermi liquid properties in Sr2RuO4 revealed by Raman spectroscopy - 17:40-20:30 (2h50)

› Overactivated transport in the localized phase of the superconductor-insulator transition - 17:40-20:30 (2h50)

› Quantum Diamond Magnetometry for High Pressure Superconductivity - 17:40-20:30 (2h50)

› Scanning tunneling spectroscopy at magnetic fields of 20T in superconducting KFe2As2 - 17:40-20:30 (2h50)

› Spectroscopic evidence for strong correlations between local superconducting gap and local Altshuler-Aronov density-of-states suppression in ultrathin NbN films - 17:40-20:30 (2h50)

› Study of superconductivity with the composite operator method - 17:40-20:30 (2h50)

› Superconductivity in novel Crystallogenide LaFeSiO with squeezed FeSi layer - 17:40-20:30 (2h50)

› Transport measurements in Megagauss fields - 17:40-20:30 (2h50)

› Upper critical field of the spin triplet superconductor UTe2 by specific heat measurements - 17:40-20:30 (2h50)

› What is the 'true' pseudogap line in cuprates ? - 17:40-20:30 (2h50)

› Superconductor-Insulator Transition in space charge doped one unit cell BiSCCO - fang wang, Institut de minéralogie, de physique des matériaux et de cosmochimie, Laboratoire de Physique et dÉtude des Matériaux (UMR 8213) 20:30-20:30 ()