Anisotropic magnetic interactions and spin dynamics in the spin-chain compound Cu(py)2Br2: An experimental and theoretical study

J. Zeisner, M. Brockmann, S. Zimmermann, A. Weiße, M. Thede, E. Ressouche, K. Yu. Povarov, A. Zheludev, A. Klümper, B. Büchner, V. Kataev, and F. Göhmann
Phys. Rev. B 96, 024429 – Published 20 July 2017

Abstract

We compare theoretical results for electron spin resonance (ESR) properties of the Heisenberg-Ising Hamiltonian with ESR experiments on the quasi-one-dimensional magnet Cu(py)2Br2 (CPB). Our measurements were performed over a wide frequency and temperature range giving insight into the spin dynamics, spin structure, and magnetic anisotropy of this compound. By analyzing the angular dependence of ESR parameters (resonance shift and linewidth) at room temperature, we show that the two weakly coupled inequivalent spin-chain types inside the compound are well described by Heisenberg-Ising chains with their magnetic anisotropy axes perpendicular to the chain direction and almost perpendicular to each other. We further determine the full g tensor from these data. In addition, the angular dependence of the linewidth at high temperatures gives us access to the exponent of the algebraic decay of a dynamical correlation function of the isotropic Heisenberg chain. From the temperature dependence of static susceptibilities, we extract the strength of the exchange coupling (J/kB=52.0K) and the anisotropy parameter (δ0.02) of the model Hamiltonian. An independent compatible value of δ is obtained by comparing the exact prediction for the resonance shift at low temperatures with high-frequency ESR data recorded at 4K. The spin structure in the ordered state implied by the two (almost) perpendicular anisotropy axes is in accordance with the propagation vector determined from neutron scattering experiments. In addition to undoped samples, we study the impact of partial substitution of Br by Cl ions on spin dynamics. From the dependence of the ESR linewidth on the doping level, we infer an effective decoupling of the anisotropic component Jδ from the isotropic exchange J in these systems.

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  • Received 25 April 2017
  • Revised 29 June 2017

DOI:https://doi.org/10.1103/PhysRevB.96.024429

©2017 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

J. Zeisner1,2, M. Brockmann3, S. Zimmermann1,2, A. Weiße4, M. Thede5, E. Ressouche6,7, K. Yu. Povarov5, A. Zheludev5, A. Klümper3, B. Büchner1,2, V. Kataev1, and F. Göhmann3

  • 1Leibniz Institute for Solid State and Materials Research IFW Dresden, D-01069 Dresden, Germany
  • 2Institute for Solid State Physics, TU Dresden, D-01069 Dresden, Germany
  • 3Department of Physics, University of Wuppertal, D-42097 Wuppertal, Germany
  • 4Max Planck Institute for Mathematics, P.O. Box 7280, D-53072 Bonn, Germany
  • 5Laboratory for Solid State Physics, ETH Zürich, 8093 Zürich, Switzerland
  • 6Université Grenoble Alpes, 38042 Grenoble, France
  • 7MEM-MDN, INAC, 38054 Grenoble, France

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Issue

Vol. 96, Iss. 2 — 1 July 2017

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