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Correlation of the superconducting critical temperature with spin and orbital excitations in (CaxLa1−x)(Ba1.75−xLa0.25+x)Cu3Oy as measured by resonant inelastic x-ray scattering

Type of publication Peer-reviewed
Publikationsform Original article (peer-reviewed)
Author Ellis David Shai, Huang Yao-Bo, Olalde-Velasco Paul, Dantz Marcus, Pelliciari Jonathan, Drachuck Gil, Ofer Rinat, Bazalitsky Galina, Berger Jorge, Schmitt Thorsten, Keren Amit,
Project Coupled spin, charge and orbital dynamics of low-dimensional cuprates
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Original article (peer-reviewed)

Journal Physical Review B
Volume (Issue) 92(10)
Page(s) 104507 - 104507
Title of proceedings Physical Review B
DOI 10.1103/physrevb.92.104507

Open Access

URL https://export.arxiv.org/abs/1508.02021
Type of Open Access Repository (Green Open Access)

Abstract

Electronic spin and orbital (dd) excitation spectra of (CaxLa1−x )(Ba1.75−xLa0.25+x)Cu3Oy samples are measured by resonant inelastic x-ray scattering (RIXS). In this compound, Tc of samples with identical hole dopings is strongly affected by the Ca/Ba substitution x due to subtle variations in the lattice constants, while crystal symmetry and disorder as measured by linewidths are x independent. We examine two extreme values of x and two extreme values of hole-doping content y corresponding to antiferromagnetic and superconducting states. The x dependence of the spin-mode energies is approximately the same for both the antiferromagnetic and superconducting samples. This clearly demonstrates that RIXS is sensitive to the superexchange J even in doped samples. A positive correlation between J and the maximum of Tc at optimal doping (T_c_max) is observed. We also measured the x dependence of the dxy → dx2−y2 and dxz/yz → dx2−y2 orbital splittings. We infer that the effect of the unresolved d3z2−r2 → dx2→y2 excitation on T_c_max is much smaller than the effect of J. There appears to be dispersion in the dxy → dx2−y2 peak of up to 0.05 eV. Our fitting furthermore indicates an asymmetric Dispersion for the dxz/yz → dx2−y2 excitation. A peak at ∼0.8 eV is also observed and attributed to a dd excitation in the chain layer.
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