超导电性
凝聚态物理
领域(数学)
材料科学
物理
数学
纯数学
作者
Willem O. Tromp,Tjerk Benschop,Jian-Feng Ge,Irene Battisti,Koen M. Bastiaans,Damianos Chatzopoulos,Amber H. M. Vervloet,Steef Smit,Erik van Heumen,M. S. Golden,Yinkai Huang,Takeshi Kondo,Tsunehiro Takeuchi,Yi Yin,Jennifer E. Hoffman,Miguel Antonio Sulangi,Jan Zaanen,Milan P. Allan
出处
期刊:Nature Materials
[Springer Nature]
日期:2023-03-06
卷期号:22 (6): 703-709
被引量:36
标识
DOI:10.1038/s41563-023-01497-1
摘要
Abstract The cuprate high-temperature superconductors exhibit many unexplained electronic phases, but the superconductivity at high doping is often believed to be governed by conventional mean-field Bardeen–Cooper–Schrieffer theory 1 . However, it was shown that the superfluid density vanishes when the transition temperature goes to zero 2,3 , in contradiction to expectations from Bardeen–Cooper–Schrieffer theory. Our scanning tunnelling spectroscopy measurements in the overdoped regime of the (Pb,Bi) 2 Sr 2 CuO 6+ δ high-temperature superconductor show that this is due to the emergence of nanoscale superconducting puddles in a metallic matrix 4,5 . Our measurements further reveal that this puddling is driven by gap filling instead of gap closing. The important implication is that it is not a diminishing pairing interaction that causes the breakdown of superconductivity. Unexpectedly, the measured gap-to-filling correlation also reveals that pair breaking by disorder does not play a dominant role and that the mechanism of superconductivity in overdoped cuprate superconductors is qualitatively different from conventional mean-field theory.
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