Your browser doesn't support javascript.
loading
Vortex Phase Dynamics in Yttrium Superhydride YH6 at Megabar Pressures.
Sadakov, Andrey V; Vlasenko, Vladimir A; Troyan, Ivan A; Sobolevskiy, Oleg A; Semenok, Dmitrii V; Zhou, Di; Pudalov, Vladimir M.
Afiliación
  • Sadakov AV; P. N. Lebedev Physical Institute, Russian Academy of Sciences, Moscow 119991, Russia.
  • Vlasenko VA; P. N. Lebedev Physical Institute, Russian Academy of Sciences, Moscow 119991, Russia.
  • Troyan IA; Shubnikov Institute of Crystallography, Federal Scientific Research Center Crystallography and Photonics, Russian Academy of Sciences, 59 Leninsky Prospekt, Moscow 119333, Russia.
  • Sobolevskiy OA; P. N. Lebedev Physical Institute, Russian Academy of Sciences, Moscow 119991, Russia.
  • Semenok DV; Center for High Pressure Science & Technology Advanced Research, Bldg. #8E, ZPark, 10 Xibeiwang East Rd, Haidian District, Beijing 100193, China.
  • Zhou D; Center for High Pressure Science & Technology Advanced Research, Bldg. #8E, ZPark, 10 Xibeiwang East Rd, Haidian District, Beijing 100193, China.
  • Pudalov VM; P. N. Lebedev Physical Institute, Russian Academy of Sciences, Moscow 119991, Russia.
J Phys Chem Lett ; 14(29): 6666-6671, 2023 Jul 27.
Article en En | MEDLINE | ID: mdl-37463103
ABSTRACT
A comprehensive study of vortex phases and vortex dynamics is presented for a recently discovered high-temperature superconductor YH6 with Tc(onset) of 215 K under a pressure of 200 GPa. The thermal activation energy (U0) is derived within the framework of the thermally activated flux flow (TAFF) theory. The activation energy yields a power law dependence U0 ∝ Hα on magnetic field with a possible crossover at a field around 8-10 T. Furthermore, we have depicted the vortex phase transition from the vortex-glass to vortex-liquid state according to the vortex-glass theory. Finally, vortex phase diagram is constructed for the first time for superhydrides. Very high estimated values of flux flow barriers U0(H) = (1.5-7) × 104 K together with high crossover fields make YH6 a rather outstanding superconductor as compared to most cuprates and iron-based systems. The Ginzburg number for YH6 Gi = (3-7) × 10-3 indicates that thermal fluctuations are not so strong and cannot broaden superconducting transitions in weak magnetic fields.

Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Idioma: En Revista: J Phys Chem Lett Año: 2023 Tipo del documento: Article País de afiliación: Rusia

Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Idioma: En Revista: J Phys Chem Lett Año: 2023 Tipo del documento: Article País de afiliación: Rusia