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Band structure of overdoped cuprate superconductors: Density functional theory matching experiments

机译:过掺杂铜酸铜超导体的带结构:密度函数理论匹配实验

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摘要

A comprehensive angle-resolved photoemission spectroscopy study of the band structure in singlelayer cuprates is presented with the aim of uncovering universal trends across different materials. Five different hole-and electron-overdoped cuprate superconductors (La1.59Eu0.2Sr0.21CuO4, La1.77Sr0.23CuO4, Bi1.74Pb0.38Sr1.88CuO6+delta, Tl2Ba2CuO6+delta, and Pr1.15La0.7Ce0.15CuO4) have been studied with special focus on the bands with a predominately d-orbital character. Using a light polarization analysis, the e(g) and t(2g) bands are identified across these materials. A clear correlation between the d(3z2-r2) band energy and the apical oxygen distance d(A) is demonstrated. Moreover, the compound dependence of the d(x2-y2) band bottom and the t(2g) band top is revealed. A direct comparison to density functional theory (DFT) calculations employing hybrid exchange-correlation functionals demonstrates excellent agreement. We thus conclude that the DFT methodology can be used to describe the global band structure of overdoped single-layer cuprates on both the hole-and electron-doped side.
机译:展示了Singlayer铜酸铜中带结构的全面的角度分辨光学激光光谱研究,目的是揭示不同材料的普遍趋势。五种不同的孔和电子oberoped铜替代超导体(La1.59eu0.2sr0.21cuo4,la1.77sr0.23cuo4,bi1.74pb0.38sr1.88cuo6 + delta,tl2ba2cuo6 + delta和pr1.15la0.7ce0.15cuo4)已经存在用主要的D-orbital角色专注于带上的特殊聚焦。使用光极化分析,鉴定e(g)和t(2g)带在这些材料上识别。对D(3Z2-R2)带能量和顶端氧距离D(A)之间的明显相关性。此外,揭示了D(X2-Y2)带底部和T(2G)带盖的复合依赖性。与密度泛函理论(DFT)计算采用混合交换相关功能的直接比较表明了良好的一致性。因此,我们得出结论,DFT方法可用于描述孔和电子掺杂侧的过掺床单层铜酸铜的全局带结构。

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  • 来源
    《Physical review》 |2019年第22期|224509.1-224509.8|共8页
  • 作者单位

    Univ Zurich Phys Inst Winterthurerstr 190 CH-8057 Zurich Switzerland;

    Univ Zurich Phys Inst Winterthurerstr 190 CH-8057 Zurich Switzerland;

    Univ Zurich Phys Inst Winterthurerstr 190 CH-8057 Zurich Switzerland;

    Chalmers Univ Technol Dept Phys SE-41296 Gothenburg Sweden;

    Univ Zurich Phys Inst Winterthurerstr 190 CH-8057 Zurich Switzerland;

    Univ Zurich Phys Inst Winterthurerstr 190 CH-8057 Zurich Switzerland|Paul Scherrer Inst Swiss Light Source CH-5232 Villigen Switzerland;

    Univ Zurich Phys Inst Winterthurerstr 190 CH-8057 Zurich Switzerland;

    Paul Scherrer Inst Swiss Light Source CH-5232 Villigen Switzerland;

    Paul Scherrer Inst Swiss Light Source CH-5232 Villigen Switzerland;

    Paul Scherrer Inst Swiss Light Source CH-5232 Villigen Switzerland|Paul Scherrer Inst Lab Muon Spin Spect CH-5232 Villigen Switzerland|Swiss Fed Inst Technol Lab Festkorperphys CH-8093 Zurich Switzerland;

    Paul Scherrer Inst Swiss Light Source CH-5232 Villigen Switzerland;

    Paul Scherrer Inst Swiss Light Source CH-5232 Villigen Switzerland;

    Paul Scherrer Inst Swiss Light Source CH-5232 Villigen Switzerland;

    Paul Scherrer Inst Swiss Light Source CH-5232 Villigen Switzerland;

    Univ Tokyo Dept Adv Mat Kashiwa Chiba 2778561 Japan;

    Univ Tokyo Dept Adv Mat Kashiwa Chiba 2778561 Japan;

    Univ Tokyo Dept Adv Mat Kashiwa Chiba 2778561 Japan;

    Sophia Univ Dept Engn & Appl Sci Tokyo 1028554 Japan;

    Tohoku Univ Dept Appl Phys Sendai Miyagi 9808579 Japan;

    Tohoku Univ Dept Appl Phys Sendai Miyagi 9808579 Japan;

    Tohoku Univ Dept Appl Phys Sendai Miyagi 9808579 Japan;

    Univ Tokyo ISSP Kashiwa Chiba 2778581 Japan;

    Univ Bristol HH Wills Phys Lab Bristol BS8 1TL Avon England;

    Univ Bristol HH Wills Phys Lab Bristol BS8 1TL Avon England;

    CROSS Tokai Ibaraki 3191106 Japan;

    Natl Inst Adv Ind Sci & Technol Elect & Photon Res Inst Tsukuba 3058568 Japan;

    Univ Zurich Phys Inst Winterthurerstr 190 CH-8057 Zurich Switzerland;

    Univ Zurich Phys Inst Winterthurerstr 190 CH-8057 Zurich Switzerland;

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