Andreas Hausoel, Simone Di Cataldo, Motoharu Kitatani, Oleg Janson, Karsten Held
{"title":"有限层镍酸盐Ndn+1NinO2n+2超导相图","authors":"Andreas Hausoel, Simone Di Cataldo, Motoharu Kitatani, Oleg Janson, Karsten Held","doi":"10.1038/s41535-025-00786-z","DOIUrl":null,"url":null,"abstract":"<p>Following the successful prediction of the superconducting phase diagram for infinite-layer nickelates, here we calculate the superconducting <i>T</i><sub>c</sub> vs. the number of layers <i>n</i> for finite-layer nickelates using the dynamical vertex approximation. To this end, we start with density functional theory, and include local correlations non-perturbatively by dynamical mean-field theory for <i>n</i> = 2–7. For all <i>n</i>, the Ni <span>\\({d}_{{x}^{2}-{y}^{2}}\\)</span> orbital crosses the Fermi level, but for <i>n</i> > 4 there are additional (<i>π</i>, <i>π</i>) pockets or tubes that slightly enhance the layer-averaged hole doping of the <span>\\({d}_{{x}^{2}-{y}^{2}}\\)</span> orbitals beyond the leading 1/<i>n</i> contribution stemming from the valence electron count. We finally calculate <i>T</i><sub>c</sub> for the single-orbital <span>\\({d}_{{x}^{2}-{y}^{2}}\\)</span> Hubbard model by dynamical vertex approximation.</p>","PeriodicalId":19283,"journal":{"name":"npj Quantum Materials","volume":"8 1","pages":""},"PeriodicalIF":5.4000,"publicationDate":"2025-07-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Superconducting phase diagram of finite-layer nickelates Ndn+1NinO2n+2\",\"authors\":\"Andreas Hausoel, Simone Di Cataldo, Motoharu Kitatani, Oleg Janson, Karsten Held\",\"doi\":\"10.1038/s41535-025-00786-z\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p>Following the successful prediction of the superconducting phase diagram for infinite-layer nickelates, here we calculate the superconducting <i>T</i><sub>c</sub> vs. the number of layers <i>n</i> for finite-layer nickelates using the dynamical vertex approximation. To this end, we start with density functional theory, and include local correlations non-perturbatively by dynamical mean-field theory for <i>n</i> = 2–7. For all <i>n</i>, the Ni <span>\\\\({d}_{{x}^{2}-{y}^{2}}\\\\)</span> orbital crosses the Fermi level, but for <i>n</i> > 4 there are additional (<i>π</i>, <i>π</i>) pockets or tubes that slightly enhance the layer-averaged hole doping of the <span>\\\\({d}_{{x}^{2}-{y}^{2}}\\\\)</span> orbitals beyond the leading 1/<i>n</i> contribution stemming from the valence electron count. We finally calculate <i>T</i><sub>c</sub> for the single-orbital <span>\\\\({d}_{{x}^{2}-{y}^{2}}\\\\)</span> Hubbard model by dynamical vertex approximation.</p>\",\"PeriodicalId\":19283,\"journal\":{\"name\":\"npj Quantum Materials\",\"volume\":\"8 1\",\"pages\":\"\"},\"PeriodicalIF\":5.4000,\"publicationDate\":\"2025-07-01\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"npj Quantum Materials\",\"FirstCategoryId\":\"88\",\"ListUrlMain\":\"https://doi.org/10.1038/s41535-025-00786-z\",\"RegionNum\":1,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q2\",\"JCRName\":\"MATERIALS SCIENCE, MULTIDISCIPLINARY\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"npj Quantum Materials","FirstCategoryId":"88","ListUrlMain":"https://doi.org/10.1038/s41535-025-00786-z","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"MATERIALS SCIENCE, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
摘要
在成功预测了无限层镍酸盐的超导相图之后,我们在这里使用动态顶点近似计算了有限层镍酸盐的超导Tc与层数n的关系。为此,我们从密度泛函理论出发,并通过动力学平均场理论包括n = 2-7的非摄动局部相关。对于所有n, Ni \({d}_{{x}^{2}-{y}^{2}}\)轨道穿过费米能级,但对于n &gt; 4,有额外的(π, π)口袋或管,这些口袋或管略微增强了\({d}_{{x}^{2}-{y}^{2}}\)轨道的层平均空穴掺杂,超出了由价电子计数产生的1/n的主要贡献。最后,我们用动态顶点逼近法计算了单轨道\({d}_{{x}^{2}-{y}^{2}}\) Hubbard模型的Tc。
Superconducting phase diagram of finite-layer nickelates Ndn+1NinO2n+2
Following the successful prediction of the superconducting phase diagram for infinite-layer nickelates, here we calculate the superconducting Tc vs. the number of layers n for finite-layer nickelates using the dynamical vertex approximation. To this end, we start with density functional theory, and include local correlations non-perturbatively by dynamical mean-field theory for n = 2–7. For all n, the Ni \({d}_{{x}^{2}-{y}^{2}}\) orbital crosses the Fermi level, but for n > 4 there are additional (π, π) pockets or tubes that slightly enhance the layer-averaged hole doping of the \({d}_{{x}^{2}-{y}^{2}}\) orbitals beyond the leading 1/n contribution stemming from the valence electron count. We finally calculate Tc for the single-orbital \({d}_{{x}^{2}-{y}^{2}}\) Hubbard model by dynamical vertex approximation.
期刊介绍:
npj Quantum Materials is an open access journal that publishes works that significantly advance the understanding of quantum materials, including their fundamental properties, fabrication and applications.