MagneticStructures and Excitations of RCrO3 (R = Y and Rare Earth Metals)

This paper investigates the magnetic structures and excitations of the orthochromites RCrO3. The neutron scattering intensities of these magnetic structures were calculated. For scenarios where the R site is non-magnetic, the Bragg peaks I(1 0 1) and I(0 1 1) are good indicators for determining the magnetic structures. On the other hand, when the R3+ sites are ordered magnetic ions, the Bragg peaks I(1 0 0) and I(0 1 0) become the indicators. This paper also discusses the magnetic excitations in RCrO3, with a particular emphasis on the spin Hamiltonian related to the Cr3+ ions. The calculations of spin-wave dispersion considering only exchange interactions indicate that the system lacks stability. Adding single-ion anisotropy stabilizes the system while creating a gap at the Γ point. The addition of the Dzyaloshinskii-Moriya interactions is necessary when the system has weak ferromagnetism, where this interaction not only widens the gap at the Γ point but also creates the gap at the zone boundary, such as [1 0 2].

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Publication Details

Journal
Quantum Beam Science
Published
2026-10-16
DOI
https://doi.org/10.3390/qubs10040024
Primary Topic
Advanced Condensed Matter Physics
Type
article
Field-Weighted Citation Impact
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article

MagneticStructures and Excitations of RCrO3 (R = Y and Rare Earth Metals)

Kaitong Sun, Yung‐Hsiang Tung, Haifeng Li, Muqing Su et al.
Quantum Beam Science
Advanced Condensed Matter Physics
article

MagneticStructures and Excitations of RCrO3 (R = Y and Rare Earth Metals)

Kaitong Sun, Yung‐Hsiang Tung, Haifeng Li, Muqing Su, S. Yano, Yinghao Zhu
article en

Abstract

This paper investigates the magnetic structures and excitations of the orthochromites RCrO3. The neutron scattering intensities of these magnetic structures were calculated. For scenarios where the R site is non-magnetic, the Bragg peaks I(1 0 1) and I(0 1 1) are good indicators for determining the magnetic structures. On the other hand, when the R3+ sites are ordered magnetic ions, the Bragg peaks I(1 0 0) and I(0 1 0) become the indicators. This paper also discusses the magnetic excitations in RCrO3, with a particular emphasis on the spin Hamiltonian related to the Cr3+ ions. The calculations of spin-wave dispersion considering only exchange interactions indicate that the system lacks stability. Adding single-ion anisotropy stabilizes the system while creating a gap at the Γ point. The addition of the Dzyaloshinskii-Moriya interactions is necessary when the system has weak ferromagnetism, where this interaction not only widens the gap at the Γ point but also creates the gap at the zone boundary, such as [1 0 2].

Quantum Beam ScienceVol. 10(4)
University of Macau (MO), National Synchrotron Radiation Research Center (TW), Heinz Maier-Leibnitz Zentrum (DE)
Openalex Percentile: Top 22%
Advanced Condensed Matter Physics
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