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Atomic-scale electronic structure of the cuprate pair density wave state coexisting with superconductivity

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,...

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Detalles Bibliográficos
Autores principales: Choubey, Peayush, Joo, Sang Hyun, Fujita, K., Du, Zengyi, Edkins, S. D., Hamidian, M. H., Eisaki, H., Uchida, S., Mackenzie, A. P., Lee, Jinho, Davis, J. C. Séamus, Hirschfeld, P. J.
Formato: Online Artículo Texto
Lenguaje:English
Publicado: National Academy of Sciences 2020
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7334493/
https://www.ncbi.nlm.nih.gov/pubmed/32546526
http://dx.doi.org/10.1073/pnas.2002429117
Descripción
Sumario: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 [Formula: see text] is predicted at the terminal BiO surface of Bi(2)Sr(2)CaCu(2)O(8) 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 [Formula: see text] , the modulations of the coherence peak energy [Formula: see text] and the characteristics of Bogoliubov quasiparticle interference in scattering-wavevector space [Formula: see text]. Consistency between all these predictions and the corresponding experiments indicates that lightly hole-doped Bi(2)Sr(2)CaCu(2)O(8) 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* [Formula: see text] 19% occurs due to disappearance of this PDW.