A universal scaling relation in high-temperature superconductors

被引:218
作者
Homes, CC [1 ]
Dordevic, SV
Strongin, M
Bonn, DA
Liang, RX
Hardy, WN
Komiya, S
Ando, Y
Yu, G
Kaneko, N
Zhao, X
Greven, M
Basov, DN
Timusk, T
机构
[1] Brookhaven Natl Lab, Dept Phys, Upton, NY 11973 USA
[2] Univ British Columbia, Dept Phys & Astron, Vancouver, BC V6T 2A6, Canada
[3] Cent Res Inst Elect Power Ind, Tokyo 2018511, Japan
[4] Stanford Univ, Dept Phys, Stanford, CA 94305 USA
[5] Stanford Synchrotron Radiat Lab, Stanford, CA 94309 USA
[6] Stanford Univ, Dept Appl Phys, Stanford, CA 94305 USA
[7] Univ Calif San Diego, Dept Phys, La Jolla, CA 92093 USA
[8] McMaster Univ, Dept Phys & Astron, Hamilton, ON L8S 4M1, Canada
基金
加拿大自然科学与工程研究理事会; 美国国家航空航天局; 美国国家科学基金会;
关键词
D O I
10.1038/nature02673
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
Since the discovery of superconductivity at elevated temperatures in the copper oxide materials(1) there has been a considerable effort to find universal trends and correlations amongst physical quantities, as a clue to the origin of the superconductivity. One of the earliest patterns that emerged was the linear scaling of the superfluid density (rho(s)) with the superconducting transition temperature (T-c), which marks the onset of phase coherence. This is referred to as the Uemura relation(2), and it works reasonably well for the underdoped materials. It does not, however, describe optimally doped ( where T-c is a maximum) or overdoped materials(3). Similarly, an attempt to scale the superfluid density with the d.c. conductivity (sigma(dc)) was only partially successful(4). Here we report a simple scaling relation (rho(s) proportional to proportional to(dc)T(c), with sigma(dc) measured at approximately T-c) that holds for all tested high-T-c materials. It holds regardless of doping level, nature of dopant ( electrons versus holes), crystal structure and type of disorder(5), and direction ( parallel or perpendicular to the copper oxygen planes).
引用
收藏
页码:539 / 541
页数:3
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