Intersite Coulomb Repulsion Driven Quadrupole Instability and Magnetic Ordering in the Orbital Frustrated Ba<sub>2</sub>MgReO<sub>6</sub>

Abstract In order to calculate the multipoles in real materials with considerable intersite Coulomb interaction V , we develop a self-consistent program which starts from the first-principles calculations to solve the tight-binding Hamiltonian including onsite Coulomb repulsion U , V , and spin-orbital coupling λ . The program is applied to Ba 2 MgReO 6 to figure out the mechanism of structural instability and magnetic ordering. A comprehensive quadrupole phase diagram versus U and V with λ = 0.28 eV is calculated. Our results demonstrate that the easy-plane anisotropy and the intersite Coulomb repulsion V must be considered to remove the orbital frustration. The increase of V to &gt; 20 meV would arrange quadrupole Q x 2 – y 2 antiparallelly, accompanied by small parallel Q 3 z 2 – r 2 , and stabilize Ba 2 MgReO 6 into the body-centered tetragonal structure. Such antiparallel Q x 2 – y 2 provides a new mechanism for the Dzyaloshinskii–Moriya interaction and gives rise to the canted antiferromagnetic (CAF) state along the [110] axis. Moreover, sizable octupoles such as <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msubsup> <mml:mi>O</mml:mi> <mml:mrow> <mml:mn>21</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>31</mml:mn> </mml:mrow> </mml:msubsup> </mml:mrow> </mml:math> , <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msubsup> <mml:mi>O</mml:mi> <mml:mrow> <mml:mn>21</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>33</mml:mn> </mml:mrow> </mml:msubsup> </mml:mrow> </mml:math> , <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msubsup> <mml:mi>O</mml:mi> <mml:mrow> <mml:mn>21</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>34</mml:mn> </mml:mrow> </mml:msubsup> </mml:mrow> </mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msubsup> <mml:mi>O</mml:mi> <mml:mrow> <mml:mn>21</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>36</mml:mn> </mml:mrow> </mml:msubsup> </mml:mrow> </mml:math> are discovered for the first time in the CAF state. Our study not only provides a comprehensive understanding of the experimental results in Ba 2 MgReO 6 , but also serves as a general and useful tool for the study of multipole physics in 5d compounds.

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Journal
Chinese Physics Letters
Published
2025-05-19
DOI
https://doi.org/10.1088/0256-307x/42/7/070703
Primary Topic
Advanced Condensed Matter Physics
Type
article
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article

Intersite Coulomb Repulsion Driven Quadrupole Instability and Magnetic Ordering in the Orbital Frustrated Ba2MgReO6

Xuanye Zhang, Jinyu Zou, Gang Xu
Chinese Physics Letters
Advanced Condensed Matter Physics
article

Intersite Coulomb Repulsion Driven Quadrupole Instability and Magnetic Ordering in the Orbital Frustrated Ba2MgReO6

Xuanye Zhang, Jinyu Zou, Gang Xu
article en

Abstract

Abstract In order to calculate the multipoles in real materials with considerable intersite Coulomb interaction V , we develop a self-consistent program which starts from the first-principles calculations to solve the tight-binding Hamiltonian including onsite Coulomb repulsion U , V , and spin-orbital coupling λ . The program is applied to Ba 2 MgReO 6 to figure out the mechanism of structural instability and magnetic ordering. A comprehensive quadrupole phase diagram versus U and V with λ = 0.28 eV is calculated. Our results demonstrate that the easy-plane anisotropy and the intersite Coulomb repulsion V must be considered to remove the orbital frustration. The increase of V to &gt; 20 meV would arrange quadrupole Q x 2 – y 2 antiparallelly, accompanied by small parallel Q 3 z 2 – r 2 , and stabilize Ba 2 MgReO 6 into the body-centered tetragonal structure. Such antiparallel Q x 2 – y 2 provides a new mechanism for the Dzyaloshinskii–Moriya interaction and gives rise to the canted antiferromagnetic (CAF) state along the [110] axis. Moreover, sizable octupoles such as <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msubsup> <mml:mi>O</mml:mi> <mml:mrow> <mml:mn>21</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>31</mml:mn> </mml:mrow> </mml:msubsup> </mml:mrow> </mml:math> , <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msubsup> <mml:mi>O</mml:mi> <mml:mrow> <mml:mn>21</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>33</mml:mn> </mml:mrow> </mml:msubsup> </mml:mrow> </mml:math> , <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msubsup> <mml:mi>O</mml:mi> <mml:mrow> <mml:mn>21</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>34</mml:mn> </mml:mrow> </mml:msubsup> </mml:mrow> </mml:math> and <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:msubsup> <mml:mi>O</mml:mi> <mml:mrow> <mml:mn>21</mml:mn> </mml:mrow> <mml:mrow> <mml:mn>36</mml:mn> </mml:mrow> </mml:msubsup> </mml:mrow> </mml:math> are discovered for the first time in the CAF state. Our study not only provides a comprehensive understanding of the experimental results in Ba 2 MgReO 6 , but also serves as a general and useful tool for the study of multipole physics in 5d compounds.

Chinese Physics LettersVol. 42(7)
Huazhong University of Science and Technology (CN), Wuhan Institute of Technology (CN)
Openalex Percentile: Top 93%
Advanced Condensed Matter Physics
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