Electronic phase diagram of high-temperature copper oxide superconductors

被引:56
作者
Chatterjee, Utpal [1 ,2 ]
Ai, Dingfei [1 ]
Zhao, Junjing [1 ]
Rosenkranz, Stephan [2 ]
Kaminski, Adam [3 ,4 ]
Raffy, Helene [5 ]
Li, Zhizhong [5 ]
Kadowaki, Kazuo [6 ]
Randeria, Mohit [7 ]
Norman, Michael R. [2 ]
Campuzano, J. C. [1 ,2 ]
机构
[1] Univ Illinois, Dept Phys, Chicago, IL 60607 USA
[2] Argonne Natl Lab, Div Mat Sci, Argonne, IL 60439 USA
[3] Iowa State Univ, Ames Lab, Ames, IA 50011 USA
[4] Iowa State Univ, Dept Phys & Astron, Ames, IA 50011 USA
[5] Univ Paris 11, Phys Solides Lab, F-91405 Orsay, France
[6] Univ Tsukuba, Inst Mat Sci, Ibaraki 305, Japan
[7] Ohio State Univ, Dept Phys, Columbus, OH 43210 USA
基金
美国国家科学基金会;
关键词
cuprates; photoelectron spectroscopy; NORMAL-STATE; PSEUDOGAP STATE; FERMI-SURFACE;
D O I
10.1073/pnas.1101008108
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 order to understand the origin of high-temperature superconductivity in copper oxides, we must understand the normal state from which it emerges. Here, we examine the evolution of the normal state electronic excitations with temperature and carrier concentration in Bi2Sr2CaCu2O8+delta using angle-resolved photo-emission. In contrast to conventional superconductors, where there is a single temperature scale T-c separating the normal from the superconducting state, the high-temperature superconductors exhibit two additional temperature scales. One is the pseudogap scale T*, below which electronic excitations exhibit an energy gap. The second is the coherence scale T-coh, below which sharp spectral features appear due to increased lifetime of the excitations. We find that T* and T-coh are strongly doping dependent and cross each other near optimal doping. Thus the highest superconducting T-c emerges from an unusual normal state that is characterized by coherent excitations with an energy gap.
引用
收藏
页码:9346 / 9349
页数:4
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