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Correlation of the superconducting critical temperature with spin and orbital excitations in (CaxLa1−x)(Ba1.75−xLa 0.25+x)Cu3Oy as measured by resonant inelastic x-ray scattering

David Shai Ellis, Yao-Bo Huang, Paul Olalde-Velasco, Marcus Dantz, Jonathan Pelliciari, Gil Drachuck, Rinat Ofer, Galina Bazalitsky, Jorge Berger, Thorsten Schmitt, Amit Keren

DOI 10.1103/PhysRevB.92.104507 · Physical Review B

T1

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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 (Tcmax) 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 Tcmax 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.

Source-reported materials — not catalogue approval

FormulaReported Tc (K)Pressure (GPa)Type
(CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy

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78Pressure not reportedunknown
(CaxLa1-x)(Ba1.75-xLa0.25+x)Cu3Oy

Archive — visibility unverified

Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

46Pressure not reportedunknown
YBa2Cu3Oy

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Source-occurrence policy only; no material identity or catalogue acceptance is inferred from the formula.

—Pressure not reportedunknown

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