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Polarization-resolved Cu L3-edge resonant inelastic x-ray scattering of orbital and spin excitations in NdBa2Cu3O7δ

R. Fumagalli, L. Braicovich, M. Minola, Y. Y. Peng, K. Kummer, D. Betto, M. Rossi, E. Lefrançois, C. Morawe, M. Salluzzo, H. Suzuki, F. Yakhou, M. Le Tacon, B. Keimer, N. B. Brookes, M. Moretti Sala, and G. Ghiringhelli
Phys. Rev. B 99, 134517 – Published 23 April 2019

Abstract

High-resolution resonant inelastic x-ray scattering (RIXS) has proven particularly effective in the determination of crystal field and spin excitations in cuprates. Its strength lies in the large Cu L3 resonance and in the fact that the scattering cross section follows quite closely the single-ion model predictions, both in the insulating parent compounds and in the superconducting doped materials. However, the spectra become increasingly broader with (hole) doping, hence resolving and assigning spectral features has proven challenging even with the highest energy resolution experimentally achievable. Here we have overcome this limitation by measuring the polarization dependence of the RIXS spectra as a function of momentum transfer and doping in thin films of NdBa2Cu3O7δ. Besides confirming the previous assignment of dd and spin excitations (magnon, bimagnon) in the antiferromagnetic insulating parent compound, we unequivocally single out the actual spin-flip contribution at all dopings. We also demonstrate that the softening of dd excitations is mainly attributed to the shift of the xy peak to lower energy loss. These results provide a definitive assessment of the RIXS spectra of cuprates and demonstrate that RIXS measurements with polarization control are practically feasible and highly informative.

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  • Received 12 February 2019

DOI:https://doi.org/10.1103/PhysRevB.99.134517

©2019 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

R. Fumagalli1, L. Braicovich1,2, M. Minola3, Y. Y. Peng1,*, K. Kummer2, D. Betto2,†, M. Rossi1, E. Lefrançois3, C. Morawe2, M. Salluzzo4, H. Suzuki3, F. Yakhou2, M. Le Tacon5, B. Keimer3, N. B. Brookes2, M. Moretti Sala1, and G. Ghiringhelli1,6,‡

  • 1Dipartimento di Fisica, Politecnico di Milano, Piazza Leonardo da Vinci 32, I-20133 Milano, Italy
  • 2ESRF, The European Synchrotron, BP 220, F-38043, Grenoble Cedex, France
  • 3Max-Planck-Institut für Festkörperforschung, Heisenbergstr. 1, 70569 Stuttgart, Germany
  • 4CNR-SPIN, Complesso Monte Santangelo, Via Cinthia, I-80126 Napoli, Italy
  • 5Institute of Solid State Physics (IFP), Karlsruhe Institute of Technology, D-76021 Karlsruhe, Germany
  • 6CNR-SPIN, Dipartimento di Fisica, Politecnico di Milano, 20133 Milano, Italy

  • *Present address: Department of Physics and Seitz Materials Research Laboratory, University of Illinois, Urbana, IL 61801, USA.
  • Present address: Max-Planck-Institut für Festkörperforschung, Heisenbergstr. 1, 70569 Stuttgart, Germany.
  • giacomo.ghiringhelli@polimi.it

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Issue

Vol. 99, Iss. 13 — 1 April 2019

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