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Three interaction energy scales in single-layer high-T\\(_C\\) cuprate HgBa\\(_2\\)CuO\\(_{4+\\delta}\\)
Three interaction energy scales in single-layer high-T\\(_C\\) cuprate HgBa\\(_2\\)CuO\\(_{4+\\delta}\\)
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Three interaction energy scales in single-layer high-T\\(_C\\) cuprate HgBa\\(_2\\)CuO\\(_{4+\\delta}\\)
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Three interaction energy scales in single-layer high-T\\(_C\\) cuprate HgBa\\(_2\\)CuO\\(_{4+\\delta}\\)
Three interaction energy scales in single-layer high-T\\(_C\\) cuprate HgBa\\(_2\\)CuO\\(_{4+\\delta}\\)

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Three interaction energy scales in single-layer high-T\\(_C\\) cuprate HgBa\\(_2\\)CuO\\(_{4+\\delta}\\)
Three interaction energy scales in single-layer high-T\\(_C\\) cuprate HgBa\\(_2\\)CuO\\(_{4+\\delta}\\)
Paper

Three interaction energy scales in single-layer high-T\\(_C\\) cuprate HgBa\\(_2\\)CuO\\(_{4+\\delta}\\)

M Yi,
2020
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Overview
The lamellar cuprate superconductors exhibit the highest ambient-pressure superconducting transition temperatures (T\\(_C\\)) and, after more than three decades of extraordinary research activity, continue to pose formidable scientific challenges. A major experimental obstacle has been to distinguish universal phenomena from materials- or technique-dependent ones. Angle-resolved photoemission spectroscopy (ARPES) measures momentum-dependent single-particle electronic excitations and has been invaluable in the endeavor to determine the anisotropic momentum-space properties of the cuprates. HgBa\\(_2\\)CuO\\(_{4+\\delta}\\) (Hg1201) is a single-CuO\\(_2\\)-layer cuprate with a particularly high optimal T\\(_C\\) and a simple crystal structure; yet there exists little information from ARPES about the electronic properties of this model system. Here we present an ARPES study of doping-, temperature-, and momentum-dependent systematics of near-nodal dispersion anomalies in Hg1201. The data reveal a hierarchy of three distinct energy scales -a sub-gap low-energy kink, an intermediate-energy kink near 55 meV, and a peak-dip-hump structure. The first two features are attributed to the coupling of electrons to Ba-derived optical phonons and in-plane bond-stretching phonons, respectively. The nodal peak-dip-hump structure appears to have a common doping-dependence in several single-layer cuprates, and is interpreted as a manifestation of pseudogap physics at the node. These results establish several universal phenomena, both in terms of connecting multiple experimental techniques for a single material, and in terms of connecting comparable spectral features in multiple structurally similar cuprates.
Publisher
Cornell University Library, arXiv.org