Raman and ARPES combined study on the connection between the existence of the pseudogap and the topology of the Fermi surface in Bi2Sr2CaCu2O8+δ

被引:14
|
作者
Loret, B. [1 ]
Gallais, Y. [1 ]
Cazayous, M. [1 ]
Zhong, R. D. [2 ]
Schneeloch, J. [2 ]
Gu, G. D. [2 ]
Fedorov, A. [3 ]
Kim, T. K. [4 ]
Borisenko, S. V. [3 ]
Sacuto, A. [1 ]
机构
[1] Univ Paris Diderot Paris 7, Lab Mat & Phenomenes Quant, CNRS, UMR 7162, F-75205 Paris 13, France
[2] Brookhaven Natl Lab, Matter Phys & Mat Sci, Upton, NY 11973 USA
[3] IFW Dresden, Helmholtzstr 20, D-01069 Dresden, Germany
[4] Diamond Light Source, Harwell Campus, Didcot OX11 0DE, Oxon, England
关键词
ANGLE-RESOLVED PHOTOEMISSION; CRITICAL-POINT; CUPRATE SUPERCONDUCTOR; PHASE-DIAGRAM; C-AXIS; YBA2CU3O6+X; TRANSITIONS; COMPETITION; DEPENDENCE; SCATTERING;
D O I
10.1103/PhysRevB.97.174521
中图分类号
T [工业技术];
学科分类号
08 ;
摘要
We study the behavior of the pseudogap in overdoped Bi2Sr2CaCu2O8+delta by electronic Raman scattering (ERS) and angle-resolved photoemission spectroscopy (ARPES) on the same single crystals. Using both techniques we find that, unlike the superconducting gap, the pseudogap related to the antibonding band vanishes above the critical doping p(c) = 0.22. Concomitantly, we show from ARPES measurements that the Fermi surface of the antibonding band is holelike below p(c) and becomes electronlike above p(c). This reveals that the existence of the pseudogap depends on the Fermi surface topology in Bi2Sr2CaCu2O8+delta, and more generally, puts strong constraint on theories of the pseudogap phase.
引用
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页数:6
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