<i>B</i> -Site-Tuned Curie Temperature and Band Gap in Half-Metallic LaCu <sub>3</sub> <i>B</i> <sub>2</sub> Re <sub>2</sub> O <sub>12</sub> ( <i>B</i> = Fe, Co, Ni) Quadruple Perovskite Oxides

An <i>A</i>- and <i>B</i>-site-ordered quadruple perovskite oxide LaCu<sub>3</sub>Ni<sub>2</sub>Re<sub>2</sub>O<sub>12</sub> was synthesized at 9 GPa and 1323 K. The crystal structure adopts a cubic space group of <i>Pn</i>-3 with the lattice constant <i>a</i> = 7.4961(1) Å. Bond valence sum calculation and X-ray absorption spectroscopy suggest the charge distribution to be La<sup>3+</sup>Cu<sup>2+</sup><sub>3</sub>Ni<sup>2+</sup><sub>2</sub>Re<sup>5.5+</sup><sub>2</sub>O<sub>12</sub>. A ferrimagnetic transition arising from the Cu<sup>2+</sup>(↑)-Ni<sup>2+</sup>(↑)-Re<sup>5.5+</sup>(↓) spin coupling is found to occur at a Curie temperature of <i>T</i><sub>C</sub> ≈ 210 K. First-principles calculations suggest a half-metallic electronic band structure for LaCu<sub>3</sub>Ni<sub>2</sub>Re<sub>2</sub>O<sub>12</sub> with an energy gap of about 1.9 eV at the up-spin channel and a conducting band at the down-spin channel. By comparison with other isostructural LaCu<sub>3</sub><i>B</i><sub>2</sub>Re<sub>2</sub>O<sub>12</sub> (<i>B</i> = Fe, Co, Ni) perovskites, we find that the electronic configuration of Re dominates the Curie temperature, as well as the half-metallic band gap.

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Journal
Inorganic Chemistry
Published
2026-02-03
DOI
https://doi.org/10.1021/acs.inorgchem.5c05176
Primary Topic
Physics of Superconductivity and Magnetism
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article
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article

B -Site-Tuned Curie Temperature and Band Gap in Half-Metallic LaCu 3 B 2 Re 2 O 12 ( B = Fe, Co, Ni) Quadruple Perovskite Oxides

Youwen Long, Shuai Tang, S. V. Streltsov, Fedor Temnikov et al.
Inorganic Chemistry
Physics of Superconductivity and Magnetism
article

B -Site-Tuned Curie Temperature and Band Gap in Half-Metallic LaCu 3 B 2 Re 2 O 12 ( B = Fe, Co, Ni) Quadruple Perovskite Oxides

Youwen Long, Shuai Tang, S. V. Streltsov, Fedor Temnikov, Alexey V. Ushakov, Zhao Pan, Zhehong Liu, Xubin Ye, Chien-Te Chen, Zhiwei Hu, Chang-Yang Kuo
article en

Abstract

An <i>A</i>- and <i>B</i>-site-ordered quadruple perovskite oxide LaCu<sub>3</sub>Ni<sub>2</sub>Re<sub>2</sub>O<sub>12</sub> was synthesized at 9 GPa and 1323 K. The crystal structure adopts a cubic space group of <i>Pn</i>-3 with the lattice constant <i>a</i> = 7.4961(1) Å. Bond valence sum calculation and X-ray absorption spectroscopy suggest the charge distribution to be La<sup>3+</sup>Cu<sup>2+</sup><sub>3</sub>Ni<sup>2+</sup><sub>2</sub>Re<sup>5.5+</sup><sub>2</sub>O<sub>12</sub>. A ferrimagnetic transition arising from the Cu<sup>2+</sup>(↑)-Ni<sup>2+</sup>(↑)-Re<sup>5.5+</sup>(↓) spin coupling is found to occur at a Curie temperature of <i>T</i><sub>C</sub> ≈ 210 K. First-principles calculations suggest a half-metallic electronic band structure for LaCu<sub>3</sub>Ni<sub>2</sub>Re<sub>2</sub>O<sub>12</sub> with an energy gap of about 1.9 eV at the up-spin channel and a conducting band at the down-spin channel. By comparison with other isostructural LaCu<sub>3</sub><i>B</i><sub>2</sub>Re<sub>2</sub>O<sub>12</sub> (<i>B</i> = Fe, Co, Ni) perovskites, we find that the electronic configuration of Re dominates the Curie temperature, as well as the half-metallic band gap.

Inorganic ChemistryVol. 65(6)
National Yang Ming Chiao Tung University (TW), Chinese Academy of Sciences (CN), National Synchrotron Radiation Research Center (TW), Max Planck Institute for Chemical Physics of Solids (DE), FZU ‒ Institute of Physics of the Academy of Sciences of the Czech Republic (CZ), National Laboratory for Superconductivity (CN), University of Chinese Academy of Sciences (CN)
Openalex Percentile: Top 66%
Physics of Superconductivity and Magnetism
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