Toward an Ab Initio Theory of High-Temperature Superconductors: A Study of Multilayer Cuprates

IF 11.6 1区 物理与天体物理 Q1 PHYSICS, MULTIDISCIPLINARY
Benjamin Bacq-Labreuil, Benjamin Lacasse, A.-M. S. Tremblay, David Sénéchal, Kristjan Haule
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To demonstrate the capabilities of our approach, we take on the challenge of explaining the remarkable physics of multilayer cuprates by focusing on the two representative Ca</a:mi></a:mrow>(</a:mo>1</a:mn>+</a:mo>n</a:mi>)</a:mo></a:mrow></a:msub>Cu</a:mi></a:mrow>n</a:mi></a:mrow></a:msub></a:mrow>O</a:mi></a:mrow>2</a:mn>n</a:mi></a:mrow></a:msub>Cl</a:mi></a:mrow>2</a:mn></a:mrow></a:msub></a:mrow></a:mrow></a:mrow></a:math> and <f:math xmlns:f=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><f:mrow><f:msub><f:mrow><f:mi>HgBa</f:mi></f:mrow><f:mrow><f:mn>2</f:mn></f:mrow></f:msub></f:mrow><f:mrow><f:msub><f:mrow><f:mi>Ca</f:mi></f:mrow><f:mrow><f:mo stretchy=\"false\">(</f:mo><f:mi>n</f:mi><f:mo>−</f:mo><f:mn>1</f:mn><f:mo stretchy=\"false\">)</f:mo></f:mrow></f:msub><f:mrow><f:msub><f:mrow><f:mi>Cu</f:mi></f:mrow><f:mrow><f:mi>n</f:mi></f:mrow></f:msub></f:mrow><f:mrow><f:msub><f:mrow><f:mi mathvariant=\"normal\">O</f:mi></f:mrow><f:mrow><f:mo stretchy=\"false\">(</f:mo><f:mn>2</f:mn><f:mi>n</f:mi><f:mo>+</f:mo><f:mn>2</f:mn><f:mo stretchy=\"false\">)</f:mo></f:mrow></f:msub></f:mrow></f:mrow></f:math> families. We shed light on the microscopic origin of many salient features of multilayer cuprates, in particular, the <m:math xmlns:m=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><m:mi>n</m:mi></m:math> dependence of their superconducting properties. The growth of <o:math xmlns:o=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><o:msub><o:mi>T</o:mi><o:mi>c</o:mi></o:msub></o:math> from the single-layer to the trilayer compounds is here explained by the reduction of the charge transfer gap and, consequently, the growth of superexchange <q:math xmlns:q=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><q:mi>J</q:mi></q:math> as <s:math xmlns:s=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><s:mi>n</s:mi></s:math> increases. The origin of both is traced to the appearance of low-energy conduction bands reminiscent of standing wave modes confined within the stack of <u:math xmlns:u=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><u:mrow><u:msub><u:mrow><u:mi>CuO</u:mi></u:mrow><u:mrow><u:mn>2</u:mn></u:mrow></u:msub></u:mrow></u:math> planes. We interpret the ultimate drop of <w:math xmlns:w=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><w:msub><w:mi>T</w:mi><w:mi>c</w:mi></w:msub></w:math> for <y:math xmlns:y=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><y:mi>n</y:mi><y:mo>≥</y:mo><y:mn>4</y:mn></y:math> as a consequence of the inhomogeneous doping between the CuO</ab:mi></ab:mrow>2</ab:mn></ab:mrow></ab:msub></ab:mrow></ab:math> planes, which prevents the emergence of superconductivity in the inner planes due to their insufficient effective hole doping, as we also highlight the existence of a minimal doping (4%) required for superconductivity to appear in one of the planes. We explain material-specific properties such as the larger propensity of <cb:math xmlns:cb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><cb:mrow><cb:msub><cb:mrow><cb:mi>HgBa</cb:mi></cb:mrow><cb:mrow><cb:mn>2</cb:mn></cb:mrow></cb:msub></cb:mrow><cb:mrow><cb:msub><cb:mrow><cb:mi>Ca</cb:mi></cb:mrow><cb:mrow><cb:mo stretchy=\"false\">(</cb:mo><cb:mi>n</cb:mi><cb:mo>−</cb:mo><cb:mn>1</cb:mn><cb:mo stretchy=\"false\">)</cb:mo></cb:mrow></cb:msub><cb:mrow><cb:msub><cb:mrow><cb:mi>Cu</cb:mi></cb:mrow><cb:mrow><cb:mi>n</cb:mi></cb:mrow></cb:msub></cb:mrow><cb:mrow><cb:msub><cb:mrow><cb:mi mathvariant=\"normal\">O</cb:mi></cb:mrow><cb:mrow><cb:mo stretchy=\"false\">(</cb:mo><cb:mn>2</cb:mn><cb:mi>n</cb:mi><cb:mo>+</cb:mo><cb:mn>2</cb:mn><cb:mo stretchy=\"false\">)</cb:mo></cb:mrow></cb:msub></cb:mrow></cb:mrow></cb:math> to superconduct compared with <jb:math xmlns:jb=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><jb:mrow><jb:msub><jb:mrow><jb:mi>Ca</jb:mi></jb:mrow><jb:mrow><jb:mo stretchy=\"false\">(</jb:mo><jb:mn>1</jb:mn><jb:mo>+</jb:mo><jb:mi>n</jb:mi><jb:mo stretchy=\"false\">)</jb:mo></jb:mrow></jb:msub><jb:mrow><jb:msub><jb:mrow><jb:mi>Cu</jb:mi></jb:mrow><jb:mrow><jb:mi>n</jb:mi></jb:mrow></jb:msub></jb:mrow><jb:mrow><jb:msub><jb:mrow><jb:mi mathvariant=\"normal\">O</jb:mi></jb:mrow><jb:mrow><jb:mn>2</jb:mn><jb:mi>n</jb:mi></jb:mrow></jb:msub><jb:mrow><jb:msub><jb:mrow><jb:mi>Cl</jb:mi></jb:mrow><jb:mrow><jb:mn>2</jb:mn></jb:mrow></jb:msub></jb:mrow></jb:mrow></jb:mrow></jb:math>. We also find the coexistence of arcs and pockets observed with photoemission, the charge redistribution between copper and oxygen, and the link to the pseudogap. Our work establishes a framework for comprehensive studies of high-temperature superconducting cuprates, enables detailed comparisons with experiment, and, through its settings, unlocks opportunities for theoretical material design of high-temperature superconductors. <jats:supplementary-material> <jats:copyright-statement>Published by the American Physical Society</jats:copyright-statement> <jats:copyright-year>2025</jats:copyright-year> </jats:permissions> </jats:supplementary-material>","PeriodicalId":20161,"journal":{"name":"Physical Review X","volume":"58 1","pages":""},"PeriodicalIF":11.6000,"publicationDate":"2025-05-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Physical Review X","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1103/physrevx.15.021071","RegionNum":1,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"PHYSICS, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0

Abstract

Significant progress toward a theory of high-temperature superconductivity in cuprates has been achieved via the study of effective one- and three-band Hubbard models. Nevertheless, material-specific predictions, while essential for constructing a comprehensive theory, remain challenging due to the complex relationship between real materials and the parameters of the effective models. By combining cluster dynamical mean-field theory and density functional theory in a charge-self-consistent manner, here we show that the goal of material-specific predictions for high-temperature superconductors from first principles is within reach. To demonstrate the capabilities of our approach, we take on the challenge of explaining the remarkable physics of multilayer cuprates by focusing on the two representative Ca(1+n)CunO2nCl2 and HgBa2Ca(n1)CunO(2n+2) families. We shed light on the microscopic origin of many salient features of multilayer cuprates, in particular, the n dependence of their superconducting properties. The growth of Tc from the single-layer to the trilayer compounds is here explained by the reduction of the charge transfer gap and, consequently, the growth of superexchange J as n increases. The origin of both is traced to the appearance of low-energy conduction bands reminiscent of standing wave modes confined within the stack of CuO2 planes. We interpret the ultimate drop of Tc for n4 as a consequence of the inhomogeneous doping between the CuO2 planes, which prevents the emergence of superconductivity in the inner planes due to their insufficient effective hole doping, as we also highlight the existence of a minimal doping (4%) required for superconductivity to appear in one of the planes. We explain material-specific properties such as the larger propensity of HgBa2Ca(n1)CunO(2n+2) to superconduct compared with Ca(1+n)CunO2nCl2. We also find the coexistence of arcs and pockets observed with photoemission, the charge redistribution between copper and oxygen, and the link to the pseudogap. Our work establishes a framework for comprehensive studies of high-temperature superconducting cuprates, enables detailed comparisons with experiment, and, through its settings, unlocks opportunities for theoretical material design of high-temperature superconductors. Published by the American Physical Society 2025
高温超导体的从头算理论:多层铜酸盐的研究
通过对有效的一波段和三波段Hubbard模型的研究,在铜酸盐高温超导理论方面取得了重大进展。然而,特定材料的预测虽然对构建一个全面的理论至关重要,但由于实际材料与有效模型参数之间的复杂关系,仍然具有挑战性。通过以电荷自洽的方式结合簇动力学平均场理论和密度泛函理论,我们证明了从第一原理对高温超导体进行特定材料预测的目标是可以实现的。为了证明我们的方法的能力,我们通过关注两个具有代表性的Ca(1+n)CunO2nCl2和HgBa2Ca(n−1)CunO(2n+2)家族来解释多层铜酸盐的非凡物理特性。我们阐明了多层铜酸盐的许多显著特征的微观起源,特别是它们的超导性质的n依赖关系。Tc从单层化合物到三层化合物的生长可以用电荷转移间隙的减小来解释,因此,超交换J和n的生长增加。两者的起源都可以追溯到低能传导带的出现,这让人联想到局限在CuO2平面堆叠中的驻波模式。我们将n≥4时Tc的最终下降解释为CuO2平面之间的不均匀掺杂的结果,由于它们的有效空穴掺杂不足,这阻止了内部平面中超导性的出现,因为我们还强调了在其中一个平面中出现超导性所需的最小掺杂(4%)的存在。我们解释了材料的特定性质,例如与Ca(1+n)CunO2nCl2相比,HgBa2Ca(n−1)CunO(2n+2)具有更大的超导倾向。我们还发现了在光发射、铜和氧之间的电荷再分配以及与赝隙的联系中观察到的弧和口袋的共存。我们的工作为高温超导铜酸盐的全面研究建立了框架,实现了与实验的详细比较,并通过其设置为高温超导体的理论材料设计提供了机会。2025年由美国物理学会出版
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来源期刊
Physical Review X
Physical Review X PHYSICS, MULTIDISCIPLINARY-
CiteScore
24.60
自引率
1.60%
发文量
197
审稿时长
3 months
期刊介绍: Physical Review X (PRX) stands as an exclusively online, fully open-access journal, emphasizing innovation, quality, and enduring impact in the scientific content it disseminates. Devoted to showcasing a curated selection of papers from pure, applied, and interdisciplinary physics, PRX aims to feature work with the potential to shape current and future research while leaving a lasting and profound impact in their respective fields. Encompassing the entire spectrum of physics subject areas, PRX places a special focus on groundbreaking interdisciplinary research with broad-reaching influence.
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