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氧化铜高温超导体中旋转对称的自发破缺。

Spontaneous breaking of rotational symmetry in copper oxide superconductors.

机构信息

Brookhaven National Laboratory, Upton, New York 11973-5000, USA.

Yale University, Applied Physics Department, New Haven, Connecticut 06520, USA.

出版信息

Nature. 2017 Jul 26;547(7664):432-435. doi: 10.1038/nature23290.

Abstract

The origin of high-temperature superconductivity in copper oxides and the nature of the 'normal' state above the critical temperature are widely debated. In underdoped copper oxides, this normal state hosts a pseudogap and other anomalous features; and in the overdoped materials, the standard Bardeen-Cooper-Schrieffer description fails, challenging the idea that the normal state is a simple Fermi liquid. To investigate these questions, we have studied the behaviour of single-crystal LaSrCuO films through which an electrical current is being passed. Here we report that a spontaneous voltage develops across the sample, transverse (orthogonal) to the electrical current. The dependence of this voltage on probe current, temperature, in-plane device orientation and doping shows that this behaviour is intrinsic, substantial, robust and present over a broad range of temperature and doping. If the current direction is rotated in-plane by an angle ϕ, the transverse voltage oscillates as sin(2ϕ), breaking the four-fold rotational symmetry of the crystal. The amplitude of the oscillations is strongly peaked near the critical temperature for superconductivity and decreases with increasing doping. We find that these phenomena are manifestations of unexpected in-plane anisotropy in the electronic transport. The films are very thin and epitaxially constrained to be tetragonal (that is, with four-fold symmetry), so one expects a constant resistivity and zero transverse voltage, for every ϕ. The origin of this anisotropy is purely electronic-the so-called electronic nematicity. Unusually, the nematic director is not aligned with the crystal axes, unless a substantial orthorhombic distortion is imposed. The fact that this anisotropy occurs in a material that exhibits high-temperature superconductivity may not be a coincidence.

摘要

铜氧化物高温超导的起源以及临界温度以上“正常”态的性质存在广泛争议。在欠掺杂的铜氧化物中,这个正常态存在赝能隙和其他异常特征;而在过掺杂的材料中,标准的 Bardeen-Cooper-Schrieffer 描述失效,挑战了正常态是简单费米液体的观点。为了研究这些问题,我们研究了通过电流的单晶 LaSrCuO 薄膜的行为。在这里,我们报告了在样品中自发产生的电压,该电压横向(正交)于电流。该电压对探针电流、温度、面内器件取向和掺杂的依赖性表明,这种行为是固有、显著、稳健的,存在于较宽的温度和掺杂范围内。如果电流方向在面内旋转一个角度 ϕ,则横向电压会以 sin(2ϕ) 形式振荡,破坏晶体的四重旋转对称性。振荡的幅度在超导临界温度附近强烈峰值,并随掺杂的增加而减小。我们发现这些现象是电子输运中意想不到的面内各向异性的表现。薄膜非常薄,并且外延限制为四方(即具有四重对称性),因此对于每个 ϕ,都期望有恒定的电阻率和零横向电压。这种各向异性的起源纯粹是电子的,即所谓的电子向列性。不同寻常的是,除非施加了相当大的正交畸变,否则向列指向不会与晶体轴对齐。这种各向异性出现在表现出高温超导性的材料中,这可能并非巧合。

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