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Unveiling the Superconducting Mechanism of Ba_{0.51}K_{0.49}BiO_{3}.
Wen, C H P; Xu, H C; Yao, Q; Peng, R; Niu, X H; Chen, Q Y; Liu, Z T; Shen, D W; Song, Q; Lou, X; Fang, Y F; Liu, X S; Song, Y H; Jiao, Y J; Duan, T F; Wen, H H; Dudin, P; Kotliar, G; Yin, Z P; Feng, D L.
Afiliação
  • Wen CHP; State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200438, People's Republic of China.
  • Xu HC; State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200438, People's Republic of China.
  • Yao Q; State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200438, People's Republic of China.
  • Peng R; State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200438, People's Republic of China.
  • Niu XH; State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200438, People's Republic of China.
  • Chen QY; Science and Technology on Surface Physics and Chemistry Laboratory, Mianyang 621908, China.
  • Liu ZT; CAS Center for Excellence in Superconducting Electronics (CENSE), Shanghai 200050, China.
  • Shen DW; State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology (SIMIT), Chinese Academy of Sciences, Shanghai 200050, China.
  • Song Q; CAS Center for Excellence in Superconducting Electronics (CENSE), Shanghai 200050, China.
  • Lou X; State Key Laboratory of Functional Materials for Informatics, Shanghai Institute of Microsystem and Information Technology (SIMIT), Chinese Academy of Sciences, Shanghai 200050, China.
  • Fang YF; State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200438, People's Republic of China.
  • Liu XS; State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200438, People's Republic of China.
  • Song YH; State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200438, People's Republic of China.
  • Jiao YJ; State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200438, People's Republic of China.
  • Duan TF; State Key Laboratory of Surface Physics, Department of Physics, and Laboratory of Advanced Materials, Fudan University, Shanghai 200438, People's Republic of China.
  • Wen HH; National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China.
  • Dudin P; Collaborative Innovation Center of Advanced Microstructures, Nanjing 210093, China.
  • Kotliar G; National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China.
  • Yin ZP; Collaborative Innovation Center of Advanced Microstructures, Nanjing 210093, China.
  • Feng DL; National Laboratory of Solid State Microstructures and Department of Physics, Nanjing University, Nanjing 210093, China.
Phys Rev Lett ; 121(11): 117002, 2018 Sep 14.
Article em En | MEDLINE | ID: mdl-30265111
ABSTRACT
The mechanism of high superconducting transition temperatures (T_{c}) in bismuthates remains under debate despite more than 30 years of extensive research. Our angle-resolved photoemission spectroscopy studies on Ba_{0.51}K_{0.49}BiO_{3} reveal an unexpectedly 34% larger bandwidth than in conventional density functional theory calculations. This can be reproduced by calculations that fully account for long-range Coulomb interactions-the first direct demonstration of bandwidth expansion due to the Fock exchange term, a long-accepted and yet uncorroborated fundamental effect in many body physics.Furthermore, we observe an isotropic superconducting gap with 2Δ_{0}/k_{B}T_{c}=3.51±0.05, and strong electron-phonon interactions with a coupling constant λ∼1.3±0.2. These findings solve a long-standing mystery-Ba_{0.51}K_{0.49}BiO_{3} is an extraordinary Bardeen-Cooper-Schrieffer superconductor, where long-range Coulomb interactions expand the bandwidth, enhance electron-phonon coupling, and generate the high T_{c}. Such effects will also be critical for finding new superconductors.

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2018 Tipo de documento: Article

Texto completo: 1 Coleções: 01-internacional Base de dados: MEDLINE Idioma: En Ano de publicação: 2018 Tipo de documento: Article