(Translated by https://www.hiragana.jp/)
Phys. Rev. B 72, 081102(R) (2005) - Anisotropic intermediate valence in ${\mathrm{Yb}}_{2}{M}_{3}{\mathrm{Ga}}_{9}$ ($M=\mathrm{Rh}$,Ir)
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Anisotropic intermediate valence in Yb2M3Ga9 (M=Rh,Ir)

A. D. Christianson, J. M. Lawrence, A. M. Lobos, A. A. Aligia, E. D. Bauer, N. O. Moreno, C. H. Booth, E. A. Goremychkin, J. L. Sarrao, J. D. Thompson, C. D. Batista, F. R. Trouw, and M. P. Hehlen
Phys. Rev. B 72, 081102(R) – Published 29 August 2005

Abstract

The intermediate valence compounds Yb2M3Ga9 (M=Rh,Ir) exhibit an anisotropic magnetic susceptibility. We report measurements of the temperature dependence of the 4f occupation number, nf(T), for Yb2M3Ga9 as well as the magnetic inelastic neutron scattering spectrum Smag(ΔでるたE) at 12 and 300 K for Yb2Rh3Ga9. Both nf(T) and Smag(ΔでるたE) were calculated for the Anderson impurity model with crystal field terms within an approach based on the noncrossing approximation. These results corroborate the importance of crystal field effects in these materials; they also suggest that Anderson lattice effects are important to the physics of Yb2M3Ga9.

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  • Received 23 February 2005

DOI:https://doi.org/10.1103/PhysRevB.72.081102

©2005 American Physical Society

Authors & Affiliations

A. D. Christianson1,2, J. M. Lawrence1, A. M. Lobos3, A. A. Aligia3, E. D. Bauer2, N. O. Moreno2, C. H. Booth4, E. A. Goremychkin5, J. L. Sarrao2, J. D. Thompson2, C. D. Batista2, F. R. Trouw2, and M. P. Hehlen2

  • 1University of California Irvine, Irvine, California 92697, USA
  • 2Los Alamos National Laboratory, Los Alamos, New Mexico 87545, USA
  • 3Centro Atómico Bariloche and Instituto Balseiro, Comisión Nacional de Energía Atómica, 8400 S. C. de Bariloche, Argentina
  • 4Lawrence Berkeley National Laboratory, Berkeley, California 94550, USA
  • 5Argonne National Laboratory, Argonne, Illinois 60439, USA

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Issue

Vol. 72, Iss. 8 — 15 August 2005

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