Texas Center for Superconductivity, University of Houston, Houston, TX 77204.
Department of Physics, University of Houston, Houston, TX 77204.
Proc Natl Acad Sci U S A. 2019 Feb 5;116(6):2004-2008. doi: 10.1073/pnas.1819512116. Epub 2019 Jan 24.
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.
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。