Phase diagram of pressure-induced high temperature superconductor La$_{3}$Ni$_{2}$O$_{7+δ}$

Yuta Ueki, Hiroya Sakurai, Hibiki Nagata, Kazuki Yamane, Ryo Matsumoto, Kensei Terashima, Keisuke Hirose, Hiroto Ohta, Masaki Kato, Yoshihiko Takano
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Abstract

We successfully synthesized samples of La$_{3}$Ni$_{2}$O$_{7+\delta}$ ($\delta = -0.50$, $-0.16$, $0.00$, $+0.01$, and $+0.12$) and measured the resistance under extremely high pressures using a diamond anvil cell to establish the electronic phase diagram. A Mott insulating state appears at $\delta = -0.50$, where all Ni ions are divalent. With increasing oxygen content, superconductivity appears at $\delta = 0.00$ and higher, above approximately 25 GPa, passing through Anderson localization at $\delta = -0.16$. The superconducting transition temperature $T_{\mathrm{c}}$ decreases with increasing pressures for both $\delta = 0.00$ and $+0.12$, with the pressure dependence of $T_{\mathrm{c}}$ being much stronger in the latter than in the former.
压力诱导高温超导体 La$_{3}$Ni_{2}$O$_{7+δ}$ 的相图
我们成功合成了 La$_{3}$Ni$_{2}$O$_{7+\delta}$($\delta = -0.50$、$-0.16$、$0.00$、$+0.01$ 和 $+0.12$)样品,并使用金刚石砧电池测量了极高压下的电阻,从而建立了电子相图。在$\delta = -0.50$处出现了莫特绝缘态,此时所有的镍离子都是二价的。随着含氧量的增加,超导性出现在$\delta = 0.00$及更高,超过约25 GPa,在$\delta =-0.16$时通过安德森局域化。在 $\delta = 0.00$ 和 $+0.12$ 时,超导转变温度 $T_{mathrm{c}}$ 随着压力的增加而降低,其中 $T_{mathrm{c}}$ 的压力依赖性在后者比前者强得多。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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