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    Exchange interactions, anisotropy, and low-temperature magnetization reversal in NdFeO3

    Amit Kumar1,2,*, A. K. Bera1,2, Christian Balz3,4, Ivan da Silva3, and S. M. Yusuf1,2,†

    • *Contact author: amitkr@barc.gov.in
    • †Contact author: smyusuf@barc.gov.in

    Phys. Rev. B 112, 094444 – Published 22 September, 2025

    DOI: https://doi.org/10.1103/8qy2-k5cb

    Abstract

    We have gained a microscopic insight into the phenomenon of double magnetization reversal observed in the NdFeO3 perovskite compound at compensation temperatures of 6.3 K (Tcomp1) and 4.3 K (Tcomp2) through analysis of the evolutions of magnetic moments, magnetic anisotropies, and exchange interactions of Nd and Fe sublattices. This understanding stems from studies involving dc magnetization, neutron depolarization, neutron diffraction, and inelastic neutron scattering (INS) on powder and single-crystal samples. Below 8.6 K, additional (magnetic) Bragg peaks are detected in neutron diffraction patterns, corresponding to the CxFz-type Nd sublattice ordering, which entails C-type antiferromagnetic (AFM) ordering along the a axis and a ferromagnetic (FM) component along the c axis. The FM components (Fz) of the Nd3+ and Fe3+ moments are too diminutive to be quantified accurately via powder neutron diffraction; as single-crystal dc magnetization study estimates the FM component (along the c axis) to be approximately 0.09 μB at 2 K. Our INS investigations on single-crystal NdFeO3 sample have unveiled the relative orientations of the Fz components of the Nd and Fe sublattice moments. The INS spectra are found to be consistent with AFM exchange couplings between the Nd-Nd and Nd-Fe sublattices as well as for a planar anisotropy of Nd spins. At 6.3 K, a complete cancellation of the Fz components of the Nd3+ and Fe3+ moments results in Tcomp1, whereas a reversal in the sign of the total magnetic moment below 5 K leads to Tcomp2 at 4.3 K. The present comprehensive single-crystal INS investigation thus shed light on the microscopic mechanism for magnetization reversal phenomenon. This microscopic understanding of such a distinctive phenomenon has practical implications for design of magnetic memory and spin-resolving devices.

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