No Nematicity at the Onset Temperature of the Pseudogap Phase in the Cuprate Superconductor YBa2Cu3Oy

被引:3
|
作者
Grissonnanche, G. [1 ,2 ,3 ,4 ]
Cyr-Choiniere, O. [1 ,2 ]
Day, J. [5 ]
Liang, R. [5 ]
Bonn, D. A. [5 ]
Hardy, W. N. [5 ]
Doiron-Leyraud, N. [1 ,2 ]
Taillefer, L. [1 ,2 ,6 ]
机构
[1] Univ Sherbrooke, Dept Phys, Inst Quant, Sherbrooke, PQ J1K 2R1, Canada
[2] Univ Sherbrooke, RQMP, Sherbrooke, PQ J1K 2R1, Canada
[3] Cornell Univ, Lab Atom & Solid State Phys, Ithaca, NY 14853 USA
[4] Kavli Inst Cornell Nanoscale Sci, Ithaca, NY 14853 USA
[5] Univ British Columbia, Dept Phys & Astron, Vancouver, BC V6T 121, Canada
[6] Canadian Inst Adv Res, Toronto, ON M5G 1M1, Canada
基金
加拿大自然科学与工程研究理事会; 加拿大创新基金会;
关键词
DENSITY-WAVE ORDER; STATE;
D O I
10.1103/PhysRevX.13.031010
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Electronic nematicity is the spontaneous loss of rotational symmetry in a metal, without breaking translational symmetry. In the cuprate superconductors, there is experimental evidence for nematicity, but its origin remains unclear. Here we investigate the onset of nematicity in the transport of charge by means of electric and thermoelectric measurements in underdoped YBa2Cu3Oy, performed by passing the current (electrical or thermal) first along the a axis then the b axis of the orthorhombic structure in the same crystal, with a hole doping p = 0.12. Upon cooling, we observe no additional in-plane anisotropy-beyond the background anisotropy due to the CuO chains-in either the resistivity rho or the Seebeck coefficient S as the temperature T* for the onset of the pseudogap phase is crossed. We conclude that the pseudogap phase of cuprates is not nematic. However, at temperatures much lower than T*, a strong additional anisotropy is observed, most clearly in the Peltier coefficient alpha = S/rho. We interpret it as nematicity associated with the development of charge order.
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页数:8
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