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  • Letter
  • Open Access

Spin waves and magnetic Hamiltonian in the low-temperature phase of LiInCr4O8

Gøran J. Nilsen1,2,*, Rafał Wawrzyńczak3,4, Harald O. Jeschke5,†, Hannu Mutka3, Takatsugu Masuda6, Nicola Casati7, Vladimir Pomjakushin8, Zenji Hiroi6, and Yoshihiko Okamoto6

  • *Contact author: goran.nilsen@stfc.ac.uk
  • †Contact author: jeschke@okayama-u.ac.jp

Phys. Rev. B 112, L020403 – Published 14 July, 2025

DOI: https://doi.org/10.1103/wjh8-qt1x

Abstract

Transition metal spinels, particularly those containing chromium 3+ ions (Cr3+), display a rich variety of low-temperature magnetostructural states. Here, we present a combined neutron scattering, synchrotron x-ray diffraction, and density functional theory study of the frustrated “breathing pyrochlore” chromium spinel LiInCr4O8, where the adjacent Cr3+ tetrahedra alternate in magnetic interaction strength. We first establish the low-temperature tetragonal structure from the diffraction measurements. Considering the magnetic structure in light of the distortions generated by this structure, the short magnetic correlation length found in a previous study can be explained by dimensional reduction due to residual frustration. The Heisenberg Hamiltonian for the low-temperature structure is extracted using density functional theory-based energy mapping and clearly shows the partial release of frustration due to the structural transition. The first four exchanges terms dominate, and the two nearest-neighbor exchanges J and J′ in the high-temperature structure both split substantially. The full magnetic excitation spectrum obtained by inelastic neutron scattering can be accurately reproduced by a linear spin-wave theory model using the density functional exchange parameters as a starting point. However, it is found that multiple parameter sets that obey the relation (J1+J4)/(J2+J3)∼1.24, J1>J2, and J3>J4 provide an equally good description of the data. This ratio, along with the low-temperature structure, suggests that it is the distortion of the small tetrahedra that drives the magnetostructural transition.

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