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通过打破普适压力关系实现更高超导转变温度。

Higher superconducting transition temperature by breaking the universal pressure relation.

机构信息

Texas Center for Superconductivity, University of Houston, Houston, TX 77204.

Department of Physics, University of Houston, Houston, TX 77204.

出版信息

Proc Natl Acad Sci U S A. 2019 Feb 5;116(6):2004-2008. doi: 10.1073/pnas.1819512116. Epub 2019 Jan 24.

Abstract

By investigating the bulk superconducting state via dc magnetization measurements, we have discovered a common resurgence of the superconducting transition temperatures (Ts) of the monolayer BiSrCuO (Bi2201) and bilayer BiSrCaCuO (Bi2212) to beyond the maximum Ts (Ts) predicted by the universal relation between T and doping () or pressure (P) at higher pressures. The T of underdoped Bi2201 initially increases from 9.6 K at ambient to a peak at 23 K at 26 GPa and then drops as expected from the universal T-P relation. However, at pressures above 40 GPa, T rises rapidly without any sign of saturation up to 30 K at 51 GPa. Similarly, the T for the slightly overdoped Bi2212 increases after passing a broad valley between 20 and 36 GPa and reaches 90 K without any sign of saturation at 56 GPa. We have, therefore, attributed this T resurgence to a possible pressure-induced electronic transition in the cuprate compounds due to a charge transfer between the Cu 3[Formula: see text] and the O 2 bands projected from a hybrid bonding state, leading to an increase of the density of states at the Fermi level, in agreement with our density functional theory calculations. Similar T-P behavior has also been reported in the trilayer BrSrCaCuO (Bi2223). These observations suggest that higher Ts than those previously reported for the layered cuprate high-temperature superconductors can be achieved by breaking away from the universal T-P relation through the application of higher pressures.

摘要

通过直流磁化测量研究体超导态,我们发现单层 BiSrCuO(Bi2201)和双层 BiSrCaCuO(Bi2212)的超导转变温度(Ts)在更高压力下普遍重新出现在超越由 T 和掺杂()或压力(P)之间的普遍关系预测的最大 Ts(Ts)。欠掺杂 Bi2201 的 T 最初从环境中的 9.6 K 增加到 26 GPa 时的 23 K 峰值,然后按照普遍的 T-P 关系预期下降。然而,在 40 GPa 以上的压力下,T 迅速升高,没有任何饱和迹象,在 51 GPa 时高达 30 K。同样,稍过掺杂的 Bi2212 的 T 在 20 和 36 GPa 之间的宽谷之后增加,并在 56 GPa 时达到 90 K,没有任何饱和迹象。因此,我们将这种 T 回升归因于铜酸盐化合物中可能由于 Cu 3[Formula: see text]和 O 2 带之间的电荷转移而在压力下诱导的电子跃迁,这导致费米能级处的态密度增加,与我们的密度泛函理论计算一致。在三层 BrSrCaCuO(Bi2223)中也报道了类似的 T-P 行为。这些观察结果表明,通过脱离普遍的 T-P 关系并通过施加更高的压力,可以实现比层状铜酸盐高温超导体以前报道的更高的 Ts。

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