{"title":"压力诱导高温超导体 La$_{3}$Ni_{2}$O$_{7+δ}$ 的相图","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":"{\"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}","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}
Phase diagram of pressure-induced high temperature superconductor La$_{3}$Ni$_{2}$O$_{7+δ}$
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.