Phase diagram of Bi2Sr2CaCu2O8+δ revisited

被引:52
|
作者
Drozdov, I. K. [1 ]
Pletikosic, I [1 ,2 ]
Kim, C-K [1 ]
Fujita, K. [1 ]
Gu, G. D. [1 ]
Davis, J. C. Seamus [1 ,3 ]
Johnson, P. D. [1 ]
Bozovic, I [1 ]
Valla, T. [1 ]
机构
[1] Brookhaven Natl Lab, Condensed Matter Phys & Mat Sci Dept, Upton, NY 11973 USA
[2] Princeton Univ, Dept Phys, Princeton, NJ 08544 USA
[3] Cornell Univ, Dept Phys, Lab Atom & Solid State Phys, Ithaca, NY 14853 USA
来源
NATURE COMMUNICATIONS | 2018年 / 9卷
关键词
HIGH-TEMPERATURE SUPERCONDUCTOR; T-C; QUANTUM OSCILLATIONS; QUASI-PARTICLE; GAP ANISOTROPY; FERMI-SURFACE; NORMAL-STATE; PSEUDOGAP; TRANSITION; EVOLUTION;
D O I
10.1038/s41467-018-07686-w
中图分类号
O [数理科学和化学]; P [天文学、地球科学]; Q [生物科学]; N [自然科学总论];
学科分类号
07 ; 0710 ; 09 ;
摘要
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, T-c, using the assumption that the Tc dependence on doping is universal. Here, we present angle-resolved photoemission studies of Bi2Sr2CaCu2O8+delta, cleaved and annealed in vacuum or in ozone to reduce or increase the doping from the initial value corresponding to T-c = 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 2 Delta(0) = (4 +/- 1)k(B)T(c)
引用
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页数:7
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