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Higher superconducting transition temperature by breaking the universal pressure relation

机译:通过打破万能压力关系获得更高的超导转变温度

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摘要

By investigating the bulk superconducting state via dc magnetization measurements, we have discovered a common resurgence of the superconducting transition temperatures (Tcs) of the monolayer Bi2Sr2CuO6+δ (Bi2201) and bilayer Bi2Sr2CaCu2O8+δ (Bi2212) to beyond the maximum Tcs (Tc-maxs) predicted by the universal relation between Tc and doping (p) or pressure (P) at higher pressures. The Tc 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 Tc-P relation. However, at pressures above 40 GPa, Tc rises rapidly without any sign of saturation up to 30 K at 51 GPa. Similarly, the Tc 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 Tc resurgence to a possible pressure-induced electronic transition in the cuprate compounds due to a charge transfer between the Cu 3dx2y2 and the O 2p 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 Tc-P behavior has also been reported in the trilayer Br2Sr2Ca2Cu3O10+δ (Bi2223). These observations suggest that higher Tcs than those previously reported for the layered cuprate high-temperature superconductors can be achieved by breaking away from the universal Tc-P relation through the application of higher pressures.
机译:通过研究直流磁化测量的体超导状态,我们发现单层Bi2Sr2CuO6 +δ(Bi2201)和双层Bi2Sr2CaCu2O8 +δ(Bi2212)的超导转变温度(Tcs)普遍回升到最大Tcs(Tc-由Tc和较高压力下的掺杂(p)或压力(P)之间的通用关系预测。掺杂不足的Bi2201的Tc最初从环境温度下的9.6 K升高到26 GPa处的23 K的峰值,然后如通用Tc-P关系所预期的那样下降。但是,在高于40 GPa的压力下,Tc迅速上升,在51 GPa时高达30 K时没有任何饱和迹象。类似地,在22 GPa和36 GPa之间通过一个宽谷之后,稍微过量掺杂的Bi2212的Tc增大,达到90 K时在56 GPa没有任何饱和迹象。因此,我们将这种Tc回潮归因于铜酸盐化合物中可能的压力诱导的电子跃迁,这是由于Cu 3 d x 2 < mo> − y 2 和O 2p从杂化键合态投影的能带,导致费米能级的态密度增加,这与我们的密度泛函理论计算是一致的。在三层Br 2 Sr 2 Ca 2 Cu c -P行为> 3 O 10 +δ(Bi2223)。这些观察结果表明,通过打破常规的T c -P关系,可以实现比先前报道的层状铜酸盐高温超导体更高的T c s。施加更高的压力。

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