説明:
(abstract)We theoretically study the piezomagnetic effect on the altermagnetic state in κ-type molecular conductors, focusing on its nonrelativistic mechanism. By introducing shear stress as a monoclinic distortion, we evaluate variations in the ef- fective tight-binding model using first-principles calculations. Using the derived parameters, we investigate the Hubbard model and its effective Heisenberg model on the two-dimensional (distorted) κ-type lattice within mean-field approxima- tion. We show that the system exhibits the piezomagnetic effect, i.e., a net magnetization induced at finite temperatures in the undoped insulating state and both in the ground state and at finite temperatures upon doping. In a real-space pic- ture, this uniform magnetization arises from the ferrimagnetic spin structure due to inequivalent spin sites induced by lattice distortion. Meanwhile, in a momentum-space picture, it stems from the s-wave spin splitting of the electron and magnon bands, independent of spin-orbit coupling. We find that this nonrelativistic piezomagnetism remains finite, but becomes smaller in the limit of strong dimerization where the energy gap between the bonding and antibonding orbitals is infinitely large and the d-wave altermagnetic spin splitting is absent, highlighting the importance of the multi-orbital nature.
権利情報:
キーワード: Organic Altermagnet, Non-relativistic Piezomagnetic Effect
刊行年月日: 2025-08-15
出版者: Physical Society of Japan
掲載誌:
研究助成金:
原稿種別: 著者最終稿 (Accepted manuscript)
MDR DOI:
公開URL: https://doi.org/10.7566/jpsj.94.083702
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その他の識別子:
連絡先:
更新時刻: 2025-11-11 08:30:06 +0900
MDRでの公開時刻: 2025-11-11 08:22:14 +0900
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2505.07327v1.pdf
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