Negative thermal expansion, lattice dynamics, and complex magnetism in TbFeO 3

arXiv:2608.00469 · cond-mat.str-el, cond-mat.mtrl-sci · Submitted 2026-08-01 · Read on arXiv

cond-mat.str-el, cond-mat.mtrl-sci

Submitted: 2026-08-01

Updated: 2026-10-16

Comments: 22 pages, 19 figures

DOI: 10.1103/dmqs-y92y

License: http://creativecommons.org/licenses/by/4.0/

The gist: We report a temperature-dependent investigation of orthoferrite TbFeO 3 using x-ray diffraction, DC magnetization, and Raman scattering, complemented by room-temperature x-ray photoelectron

Terminology

Abstract

We report a temperature-dependent investigation of orthoferrite TbFeO 3 using x-ray diffraction, DC magnetization, and Raman scattering, complemented by room-temperature x-ray photoelectron spectroscopy. X-ray diffraction reveals negative thermal expansion over 5-300 K, with a small but systematic increase in unit-cell volume upon cooling in the absence of any structural phase transition. Raman scattering measurements identify the Raman-active phonon modes and show clear deviations from the conventional Klemens anharmonic decay model, particularly in phonon frequencies, indicating the presence of spin-phonon coupling. Two modes of A g and B 1g symmetry exhibit a crossover from Gaussian-dominated line shapes at low temperatures to mixed Gaussian-Lorentzian profiles at higher temperatures, reflecting a transition from inhomogeneous broadening to lifetime-driven dynamics. High-energy Raman spectra reveal two-magnon excitations associated with the Fe sublattice, consistent with linear spin-wave theory, whose spectral weight shows only weak temperature dependence. In addition, a broad Raman mode emerging below about 175 K exhibits an order-parameter-like temperature evolution and coincides with the onset of phonon anomalies, while no corresponding strong anomaly is observed in the two-magnon response. Taken together, these results establish TbFeO 3 as a system with pronounced interplay among lattice dynamics, spin correlations, and emergent local magnetic-lattice anomalies.

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