A case for resonant X-ray Bragg diffraction by a collinear antiferromagnet Li <sub>2</sub> Ni <sub>3</sub> P <sub>4</sub> O <sub>14</sub>

Magnetic axial and polar (Dirac) nickel multipoles contribute to resonant X-ray Bragg amplitudes in a symmetry-informed analysis of monoclinic Li<sub>2</sub>Ni<sub>3</sub>P<sub>4</sub>O<sub>14</sub> presented for future diffraction experiments. Magnetic long-range order below a temperature of ≃ 14.5 K can be viewed as a two-dimensional trimerized antiferromagnet with Ni ions in two Wyckoff positions in the centrosymmetric (1) magnetic space group P2<sub>1</sub>/c. It permits the coupling to circular polarization in the primary X-ray beam, unlike the corresponding diffraction by an antiferromagnet characterized by anti-inversion (1') and a linear magnetoelectric effect, e.g. historically significant chromium sesquioxide (Cr<sub>2</sub>O<sub>3</sub>) and Cu<sub>2</sub>(MoO<sub>4</sub>)(SeO<sub>3</sub>) [Lovesey & van der Laan (2024). Phys. Rev. B 110, 174442]. The space group is inferred from neutron Bragg diffraction patterns, without an allowance for permitted Dirac dipoles (anapoles) and quadrupoles [Chikara et al. (2025). Phys. Rev. B 112, 014438].

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Publication Details

Journal
Acta Crystallographica Section B Structural Science Crystal Engineering and Materials
Published
2025-11-07
DOI
https://doi.org/10.1107/s2052520625009485
Primary Topic
Advanced Condensed Matter Physics
Type
article
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article

A case for resonant X-ray Bragg diffraction by a collinear antiferromagnet Li 2 Ni 3 P 4 O 14

S W Lovesey
Acta Crystallographica Section B Structural Science Crystal Engineering and Materials
Advanced Condensed Matter Physics
article

A case for resonant X-ray Bragg diffraction by a collinear antiferromagnet Li 2 Ni 3 P 4 O 14

S W Lovesey
article en

Abstract

Magnetic axial and polar (Dirac) nickel multipoles contribute to resonant X-ray Bragg amplitudes in a symmetry-informed analysis of monoclinic Li<sub>2</sub>Ni<sub>3</sub>P<sub>4</sub>O<sub>14</sub> presented for future diffraction experiments. Magnetic long-range order below a temperature of ≃ 14.5 K can be viewed as a two-dimensional trimerized antiferromagnet with Ni ions in two Wyckoff positions in the centrosymmetric (1) magnetic space group P2<sub>1</sub>/c. It permits the coupling to circular polarization in the primary X-ray beam, unlike the corresponding diffraction by an antiferromagnet characterized by anti-inversion (1') and a linear magnetoelectric effect, e.g. historically significant chromium sesquioxide (Cr<sub>2</sub>O<sub>3</sub>) and Cu<sub>2</sub>(MoO<sub>4</sub>)(SeO<sub>3</sub>) [Lovesey & van der Laan (2024). Phys. Rev. B 110, 174442]. The space group is inferred from neutron Bragg diffraction patterns, without an allowance for permitted Dirac dipoles (anapoles) and quadrupoles [Chikara et al. (2025). Phys. Rev. B 112, 014438].

Acta Crystallographica Section B Structural Science Crystal Engineering and MaterialsVol. 81(6)
Diamond Light Source (GB), University of Oxford (GB)
Openalex Percentile: Top 78%
Advanced Condensed Matter Physics
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