Conical incommensurate magnetic ordering in the transition metal-rich YCo12B6 ternary boride

The ternary boride YCo 12 B 6 was investigated by means of ac susceptibility, magnetization, and neutron powder diffraction experiments over the temperature range 1.5–300 K. The crystal structure was refined and the spin configuration determined. This intermetallic compound crystalizes in a rhombohedral R 3 ¯ m structure. In the ground state, its magnetic structure is characterized by a short incommensurate propagation vector k = (0, 0, ± 0.0432), i.e., a long incommensurate period along the c -axis. Substantially different magnetic moments have been observed on the two crystallographically inequivalent Co sites (18 g and 18 h ), a larger moment being refined on the Co-18 h position. The Co spins arrange themselves into a conical magnetic structure with a tilt angle of about 57° with respect to the threefold symmetry axis c . Furthermore, a highly anisotropic lattice expansion is observed. • Neutron powder diffraction. • Long incommensurate period along the c -axis. • Spin conical modulations. • Highly anisotropic lattice expansion.

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Publication Details

Journal
Journal of Alloys and Compounds
Published
2025-07-19
DOI
https://doi.org/10.1016/j.jallcom.2025.182379
Citations
1
Primary Topic
Magnetic Properties of Alloys
Type
article
Field-Weighted Citation Impact
0.43
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article

Conical incommensurate magnetic ordering in the transition metal-rich YCo12B6 ternary boride

B. Vallet-Simond, O. Isnard, L.V.B. Diop
1 citations
Journal of Alloys and Compounds
Magnetic Properties of Alloys
0.43
article

Conical incommensurate magnetic ordering in the transition metal-rich YCo12B6 ternary boride

B. Vallet-Simond, O. Isnard, L.V.B. Diop
article en
1 citations

Abstract

The ternary boride YCo 12 B 6 was investigated by means of ac susceptibility, magnetization, and neutron powder diffraction experiments over the temperature range 1.5–300 K. The crystal structure was refined and the spin configuration determined. This intermetallic compound crystalizes in a rhombohedral R 3 ¯ m structure. In the ground state, its magnetic structure is characterized by a short incommensurate propagation vector k = (0, 0, ± 0.0432), i.e., a long incommensurate period along the c -axis. Substantially different magnetic moments have been observed on the two crystallographically inequivalent Co sites (18 g and 18 h ), a larger moment being refined on the Co-18 h position. The Co spins arrange themselves into a conical magnetic structure with a tilt angle of about 57° with respect to the threefold symmetry axis c . Furthermore, a highly anisotropic lattice expansion is observed. • Neutron powder diffraction. • Long incommensurate period along the c -axis. • Spin conical modulations. • Highly anisotropic lattice expansion.

Journal of Alloys and CompoundsVol. 1037
Centre National de la Recherche Scientifique (FR), Institut Néel (FR), Institut Jean Lamour (FR), Université Grenoble Alpes (FR), Université de Lorraine (FR)
Openalex Percentile: Top 39%
Magnetic Properties of Alloys
0.43
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