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强无序掺杂铜氧化物超导体中竞争序涨落的模拟中的鲁棒节点 d 波谱。

Robust nodal d-wave spectrum in simulations of a strongly fluctuating competing order in underdoped cuprate superconductors.

机构信息

Department of Physics and Astronomy, Trent University, Peterborough, Ontario, Canada K9J 7B8.

出版信息

Phys Rev Lett. 2012 Dec 28;109(26):267004. doi: 10.1103/PhysRevLett.109.267004. Epub 2012 Dec 27.

Abstract

We resolve an existing discrepancy between convincing evidence for competing order in underdoped cuprates and spectroscopic data consistent with a homogeneous d-wave superconductor in the very same compounds. Specifically, we show that fluctuations of the competing order generate strongly inhomogeneous states whose spectra are almost indistinguishable from the pure d-wave superconductor. This is in contrast to the commonly studied case of homogeneously coexisting order, which typically generates a reconstructed Fermi surface with closed Fermi pockets. The signatures of the fluctuating competing order can be found mainly in a splitting of the antinodal band, and, for strong magnetic order, in small induced nodal gaps similar to those found in recent experiments on underdoped La(2-x)Sr(x)CuO4.

摘要

我们解决了在欠掺杂 cuprates 中竞争有序的令人信服的证据与光谱数据之间存在的差异,这些光谱数据与同一化合物中的均匀 d 波超导体一致。具体来说,我们表明,竞争有序的涨落产生了强烈的非均匀状态,其谱几乎与纯 d 波超导体无法区分。这与通常研究的均匀共存有序的情况形成对比,均匀共存有序通常会产生具有封闭费米面的重构费米面。波动竞争有序的特征主要可以在节点带的劈裂中找到,对于强磁场有序,在小的诱导节点间隙中也可以找到,类似于最近在欠掺杂 La(2-x)Sr(x)CuO4 上进行的实验中发现的间隙。

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