{"title":"Phase diagram of pressure-induced high temperature superconductor La$_{3}$Ni$_{2}$O$_{7+δ}$","authors":"Yuta Ueki, Hiroya Sakurai, Hibiki Nagata, Kazuki Yamane, Ryo Matsumoto, Kensei Terashima, Keisuke Hirose, Hiroto Ohta, Masaki Kato, Yoshihiko Takano","doi":"arxiv-2408.04970","DOIUrl":null,"url":null,"abstract":"We successfully synthesized samples of La$_{3}$Ni$_{2}$O$_{7+\\delta}$\n($\\delta = -0.50$, $-0.16$, $0.00$, $+0.01$, and $+0.12$) and measured the\nresistance under extremely high pressures using a diamond anvil cell to\nestablish the electronic phase diagram. A Mott insulating state appears at\n$\\delta = -0.50$, where all Ni ions are divalent. With increasing oxygen\ncontent, superconductivity appears at $\\delta = 0.00$ and higher, above\napproximately 25 GPa, passing through Anderson localization at $\\delta =\n-0.16$. The superconducting transition temperature $T_{\\mathrm{c}}$ decreases\nwith increasing pressures for both $\\delta = 0.00$ and $+0.12$, with the\npressure dependence of $T_{\\mathrm{c}}$ being much stronger in the latter than\nin the former.","PeriodicalId":501069,"journal":{"name":"arXiv - PHYS - Superconductivity","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2024-08-09","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - Superconductivity","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2408.04970","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
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.