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Tunable Magnon Interactions in a Ferromagnetic Spin-1 Chain

Prashant Chauhan, Fahad Mahmood, Hitesh J. Changlani, S. M. Koohpayeh, and N. P. Armitage
Phys. Rev. Lett. 124, 037203 – Published 23 January 2020
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Abstract

NiNb2O6 is an almost ideal realization of a 1D spin-1 ferromagnetic Heisenberg chain compound with weak unidirectional anisotropy. Using time-domain THz spectroscopy, we measure the low-energy electrodynamic response of NiNb2O6 as a function of temperature and external magnetic field. At low temperatures, we find a magnonlike spin excitation, which corresponds to the lowest energy excitation at q0. At higher temperatures, we unexpectedly observe a temperature-dependent renormalization of the spin-excitation energy, which has a strong dependence on field direction. Using theoretical arguments, exact diagonalizations, and finite temperature dynamical Lanczos calculations, we construct a picture of magnon-magnon interactions that naturally explains the observed renormalization. We show how magnetic field strength and direction may be used to directly tune the sign of the magnon-magnon interaction. This unique scenario is a consequence of the spin-1 nature and has no analog in the more widely studied spin-1/2 systems.

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  • Received 15 July 2019
  • Revised 7 October 2019

DOI:https://doi.org/10.1103/PhysRevLett.124.037203

© 2020 American Physical Society

Physics Subject Headings (PhySH)

Condensed Matter, Materials & Applied Physics

Authors & Affiliations

Prashant Chauhan1, Fahad Mahmood1,*,‡, Hitesh J. Changlani2,3,1,†, S. M. Koohpayeh1, and N. P. Armitage1

  • 1The Institute for Quantum Matter, Department of Physics and Astronomy, The Johns Hopkins University, Baltimore, Maryland 21218, USA
  • 2Department of Physics, Florida State University, Tallahassee, Florida 32306, USA
  • 3National High Magnetic Field Laboratory, Tallahassee, Florida 32304, USA

  • *fahad@illinois.edu
  • hchanglani@fsu.edu
  • Present address: Department of Physics, University of Illinois at Urbana-Champaign, Urbana, Illinois 61801-3080, USA

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Vol. 124, Iss. 3 — 24 January 2020

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  • Figure 1
    Figure 1

    (a) Ni spin-1 chains along the crystallographic c axis in the bc plane of NiNb2O6. (b) Transmission amplitude as a function of frequency ν in the absence of an external field (H=0) for various temperatures. Here ka, ec, hb, where k is the wave vector of the incident THz while e and h denote its ac electric and magnetic fields, respectively. (c)–(d) Field dependence of transmission at 5 K for both transverse and longitudinal field geometries, respectively.

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  • Figure 2
    Figure 2

    (a) Field and (c) temperature dependence of the center frequency νc of the peak observed in χ2 for ka, ec, hb. Error bar in (a) represents a 95% confidence interval. Dashed lines are calculations as described in the text. (b) and (d) Imaginary part of the magnetic susceptibility χ2(ν) for various temperatures. H=68kG (Ha) in (b) while H=65kG (Hc) in (d). Dashed lines are fit to a Lorentzian. Note that the susceptibility data near the peak are unreliable in (d) due to very strong absorption. It was excluded from the plots and fits for this reason.

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  • Figure 3
    Figure 3

    Simulated excited state energy spectra (relative to the ground state) of the spin-1 chain (L=14) as a function of external magnetic field (a) along the a axis and (b) the c axis. Bold points correspond to the excited states with the size of the big circles proportionate to |Excited|Sy|Ground|2. (c)–(d) Simulated temperature dependence of normalized χ2 computed with finite temperature dynamical Lanczos at H=65 kG in both transverse and longitudinal geometries with a Lorentzian used to broaden the spectra. The normalized magnon-magnon correlator (see text) for (e) transverse (assuming the two spin flip term can be ignored, see Supplemental Material [36]) and (f) longitudinal geometries with respect to a chosen reference site (labeled as site 0), evaluated in the lowest energy 2-magnon wave function in chains of different lengths, for H=70kG. The correlator of a site with itself has been omitted.

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