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Phase diagram of Bi2Sr2CaCu2O8+δ revisited.
Drozdov, I K; Pletikosic, I; Kim, C-K; Fujita, K; Gu, G D; Davis, J C Séamus; Johnson, P D; Bozovic, I; Valla, T.
Afiliación
  • Drozdov IK; Condensed Matter Physics and Materials Science Department, Brookhaven National Lab, Upton, NY, 11973, USA.
  • Pletikosic I; Condensed Matter Physics and Materials Science Department, Brookhaven National Lab, Upton, NY, 11973, USA.
  • Kim CK; Department of Physics, Princeton University, Princeton, NJ, 08544, USA.
  • Fujita K; Condensed Matter Physics and Materials Science Department, Brookhaven National Lab, Upton, NY, 11973, USA.
  • Gu GD; Condensed Matter Physics and Materials Science Department, Brookhaven National Lab, Upton, NY, 11973, USA.
  • Davis JCS; Condensed Matter Physics and Materials Science Department, Brookhaven National Lab, Upton, NY, 11973, USA.
  • Johnson PD; Condensed Matter Physics and Materials Science Department, Brookhaven National Lab, Upton, NY, 11973, USA.
  • Bozovic I; Laboratory of Atomic and Solid State Physics, Department of Physics, Cornell University, Ithaca, NY, 14853, USA.
  • Valla T; Condensed Matter Physics and Materials Science Department, Brookhaven National Lab, Upton, NY, 11973, USA.
Nat Commun ; 9(1): 5210, 2018 12 06.
Article en En | MEDLINE | ID: mdl-30523265
ABSTRACT
In cuprate superconductors, the doping of carriers into the parent Mott insulator induces superconductivity and various other phases whose characteristic temperatures are typically plotted versus the doping level p. In most materials, p cannot be determined from the chemical composition, but it is derived from the superconducting transition temperature, Tc, using the assumption that the Tc dependence on doping is universal. Here, we present angle-resolved photoemission studies of Bi2Sr2CaCu2O8+δ, cleaved and annealed in vacuum or in ozone to reduce or increase the doping from the initial value corresponding to Tc = 91 K. We show that p can be determined from the underlying Fermi surfaces and that in-situ annealing allows mapping of a wide doping regime, covering the superconducting dome and the non-superconducting phase on the overdoped side. Our results show a surprisingly smooth dependence of the inferred Fermi surface with doping. In the highly overdoped regime, the superconducting gap approaches the value of 2Δ0 = (4 ± 1)kBTc.

Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Idioma: En Revista: Nat Commun Asunto de la revista: BIOLOGIA / CIENCIA Año: 2018 Tipo del documento: Article País de afiliación: Estados Unidos

Texto completo: 1 Colección: 01-internacional Base de datos: MEDLINE Idioma: En Revista: Nat Commun Asunto de la revista: BIOLOGIA / CIENCIA Año: 2018 Tipo del documento: Article País de afiliación: Estados Unidos
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