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Atomic-scale electronic structure of the cuprate pair density wave state coexisting with superconductivity.
Proceedings of the National Academy of Sciences of the United States of America ( IF 9.4 ) Pub Date : 2020-06-30 , DOI: 10.1073/pnas.2002429117
Peayush Choubey 1, 2 , Sang Hyun Joo 3 , K Fujita 4 , Zengyi Du 4 , S D Edkins 5 , M H Hamidian 6 , H Eisaki 7 , S Uchida 7 , A P Mackenzie 8 , Jinho Lee 3 , J C Séamus Davis 9, 10, 11 , P J Hirschfeld 12
Affiliation  

The defining characteristic of hole-doped cuprates is d-wave high temperature superconductivity. However, intense theoretical interest is now focused on whether a pair density wave state (PDW) could coexist with cuprate superconductivity [D. F. Agterberg et al., Annu. Rev. Condens. Matter Phys. 11, 231 (2020)]. Here, we use a strong-coupling mean-field theory of cuprates, to model the atomic-scale electronic structure of an eight-unit-cell periodic, d-symmetry form factor, pair density wave (PDW) state coexisting with d-wave superconductivity (DSC). From this PDW + DSC model, the atomically resolved density of Bogoliubov quasiparticle states Nr,E is predicted at the terminal BiO surface of Bi2Sr2CaCu2O8 and compared with high-precision electronic visualization experiments using spectroscopic imaging scanning tunneling microscopy (STM). The PDW + DSC model predictions include the intraunit-cell structure and periodic modulations of Nr,E, the modulations of the coherence peak energy Δpr, and the characteristics of Bogoliubov quasiparticle interference in scattering-wavevector space q-space. Consistency between all these predictions and the corresponding experiments indicates that lightly hole-doped Bi2Sr2CaCu2O8 does contain a PDW + DSC state. Moreover, in the model the PDW + DSC state becomes unstable to a pure DSC state at a critical hole density p*, with empirically equivalent phenomena occurring in the experiments. All these results are consistent with a picture in which the cuprate translational symmetry-breaking state is a PDW, the observed charge modulations are its consequence, the antinodal pseudogap is that of the PDW state, and the cuprate critical point at p* ≈ 19% occurs due to disappearance of this PDW.



中文翻译:

铜酸盐对密度波态与超导性的原子尺度电子结构。

空穴掺杂的铜酸盐的定义特征是d波高温超导。但是,现在人们对理论上的浓厚兴趣集中在线对密度波态(PDW)是否可以与铜酸盐超导性共存[DF Agterberg等人,Annu。Biol。Chem。,1993,53,1959] 。凝视牧师 物质物理学 11,231(2020)]。在这里,我们使用铜酸盐的强耦合平均场理论,对与d波共存的8单元胞周期d对称形状因子,对密度波(PDW)状态的原子尺度电子结构进行建模超导(DSC)。从这个PDW + DSC模型中,Bogoliubov准粒子态的原子分辨密度ñ[RË在Bi 2 Sr 2 CaCu 2 O 8的末端BiO表面预测了γ射线,并与使用光谱成像扫描隧道显微镜(STM)的高精度电子可视化实验进行了比较。PDW + DSC模型的预测包括单元格内结构和周期性调制ñ[RË,相干峰值能量的调制 Δp[R 波矢量空间中的波哥廖布夫准粒子干涉及其特性 q--空间。所有这些预测与相应实验之间的一致性表明,轻度掺杂Bi 2 Sr 2 CaCu 2 O 8的确包含PDW + DSC状态。此外,在该模型中,PDW + DSC状态在临界孔密度p *下变得不稳定,成为纯DSC状态,实验中出现了经验上相同的现象。所有这些结果与图片一致,在该图片中,铜酸盐的平移对称性破坏状态为PDW,观察到的电荷调制为其结果,抗结伪间隙为PDW状态,且铜酸盐的临界点为p * ≈19 %由于此PDW的消失而发生。

更新日期:2020-06-30
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