Extending Universal Nodal Excitations Optimizes Superconductivity in Bi2Sr2CaCu2O8+δ

被引:108
|
作者
Pushp, Aakash [1 ,2 ,3 ]
Parker, Colin V. [1 ,2 ]
Pasupathy, Abhay N. [1 ,2 ]
Gomes, Kenjiro K. [1 ,2 ]
Ono, Shimpei [4 ]
Wen, Jinsheng [5 ]
Xu, Zhijun [5 ]
Gu, Genda [5 ]
Yazdani, Ali [1 ,2 ]
机构
[1] Princeton Univ, Joseph Henry Labs, Princeton, NJ 08544 USA
[2] Princeton Univ, Dept Phys, Princeton, NJ 08544 USA
[3] Univ Illinois, Dept Phys, Urbana, IL 61801 USA
[4] Cent Res Inst Elect Power Ind, Tokyo 2018511, Japan
[5] Brookhaven Natl Lab, Upton, NY 11973 USA
基金
美国国家科学基金会;
关键词
HIGH-T-C; HIGH-TEMPERATURE SUPERCONDUCTORS; UNDERDOPED BI2212; MOTT INSULATOR; ENERGY GAPS; PSEUDOGAP;
D O I
10.1126/science.1174338
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
Understanding the mechanism by which d wave superconductivity in the cuprates emerges and is optimized by doping the Mott insulator is one of the major outstanding problems in condensed-matter physics. Our high-resolution scanning tunneling microscopy measurements of the high-transition temperature (T-c) superconductor Bi2Sr2CaCu2O8+delta show that samples with different T-c values in the low doping regime follow a remarkably universal d wave low-energy excitation spectrum, indicating a doping-independent nodal gap. We demonstrate that T-c instead correlates with the fraction of the Fermi surface over which the samples exhibit the universal spectrum. Optimal T-c is achieved when all parts of the Fermi surface follow this universal behavior. Increasing the temperature above T-c turns the universal spectrum into an arc of gapless excitations, whereas overdoping breaks down the universal nodal behavior.
引用
收藏
页码:1689 / 1693
页数:5
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