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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)
Publication date
2015
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
Mott Physics Beyond the Heisenberg Model in Iridates and Related Materials
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Original article (peer-reviewed)
Journal
PHYSICAL REVIEW B
Volume (Issue)
92(10)
Page(s)
104507
Title of proceedings
PHYSICAL REVIEW B
DOI
10.1103/PhysRevB.92.104507
Open Access
URL
http://infoscience.epfl.ch/record/226816
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 max c) 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 max c 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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