The first term represents the exchange coupling, while the second term corresponds to the square of the total magnetic mo- ment of the supercell

On-site magnetization term To address this, we propose the following Hamiltonian: HM = −JM X i,j Si · Sj − M N ( X i Si)2, (5) where J M, M are constants to be determined

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Magnetic Order and Strain in Hexagonal Manganese Pnictide CaMn$_2$Bi$_2$

cond-mat.mtrl-sci · 2024-10-30 · unverdicted · novelty 4.0

DFT+U+SOC calculations indicate strain-tunable easy-plane magnetic anisotropy in antiferromagnetic CaMn2Bi2, with preferred in-plane direction switchable by small strains.

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Magnetic Order and Strain in Hexagonal Manganese Pnictide CaMn$_2$Bi$_2$ cond-mat.mtrl-sci · 2024-10-30 · unverdicted · none · ref 2
DFT+U+SOC calculations indicate strain-tunable easy-plane magnetic anisotropy in antiferromagnetic CaMn2Bi2, with preferred in-plane direction switchable by small strains.

The first term represents the exchange coupling, while the second term corresponds to the square of the total magnetic mo- ment of the supercell

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