Spontaneous breaking of time-reversal symmetry in the pseudogap state of a high-Tc superconductor

被引:269
作者
Kaminski, A
Rosenkranz, S
Fretwell, HM
Campuzano, JC [1 ]
Li, Z
Raffy, H
Cullen, WG
You, H
Olson, CG
Varma, CM
Höchst, H
机构
[1] Univ Illinois, Dept Phys, Chicago, IL 60607 USA
[2] Argonne Natl Lab, Div Mat Sci, Argonne, IL 60439 USA
[3] Univ Coll Swansea, Dept Phys, Swansea SA2 8PP, W Glam, Wales
[4] Univ Paris 11, Phys Solides Lab, F-91405 Orsay, France
[5] Iowa State Univ, Ames Lab, Ames, IA 50011 USA
[6] Lucent Technol, Bell Labs, Murray Hill, NJ 07974 USA
[7] Univ Wisconsin, Ctr Synchrotron Radiat, Stoughton, WI 53589 USA
基金
美国国家科学基金会;
关键词
D O I
10.1038/416610a
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
A change in 'symmetry' is often observed when matter undergoes a phase transition-the symmetry is said to be spontaneously broken. The transition made by underdoped high-transition-temperature (high-T-c) superconductors is unusual, in that it is not a mean-field transition as seen in other superconductors. Rather, there is a region in the phase diagram above the superconducting transition temperature T-c (where phase coherence and superconductivity begin) but below a characteristic temperature T* where a 'pseudogap' appears in the spectrum of electronic excitations(1,2). It is therefore important to establish if T* is just a cross-over temperature arising from fluctuations in the order parameter that will establish superconductivity at T-c (refs 3, 4), or if it marks a phase transition where symmetry is spontaneously broken(5-10). Here we report that, for a material in the pseudogap state, left-circularly polarized photons give a different photocurrent from right-circularly polarized photons. This shows that time-reversal symmetry is spontaneously broken(11) below T*, which therefore corresponds to a phase transition.
引用
收藏
页码:610 / 613
页数:5
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