Controlling phase transition in monolayer metal diiodides XI\(_{2}\) (X: Fe, Co, and Ni) by carrier doping
We applied the generalized Bloch theorem to verify the ground state (most stable state) in monolayer metal diiodides 1T-XI\(_{2}\) (X: Fe, Co, and Ni), a family of metal dihalides, using the first-principles calculations. The ground state, which can be ferromagnetic, antiferromagnetic, or spiral sta...
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Published in | arXiv.org |
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Main Author | |
Format | Paper Journal Article |
Language | English |
Published |
Ithaca
Cornell University Library, arXiv.org
28.07.2021
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Subjects | |
Online Access | Get full text |
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Summary: | We applied the generalized Bloch theorem to verify the ground state (most stable state) in monolayer metal diiodides 1T-XI\(_{2}\) (X: Fe, Co, and Ni), a family of metal dihalides, using the first-principles calculations. The ground state, which can be ferromagnetic, antiferromagnetic, or spiral state, was specified by a wavevector in the primitive unit cell. While the ground state of FeI\(_{2}\) is ferromagnetic, the spiral state becomes the ground state for CoI\(_{2}\) and NiI\(_{2}\). Since the multiferroic behavior in the metal dihalide can be preserved by the spiral structure, we believe that CoI\(_{2}\) and NiI\(_{2}\) are promising multiferroic materials in the most stable state. When the lattice parameter increases, we also show that the ground state of NiI\(_{2}\) changes to a ferromagnetic state while others still keep their initial ground states. For the last discussion, we revealed the phase transition manipulated by hole-electron doping due to the spin-spin competition between the ferromagnetic superexchange and the antiferromagnetic direct exchange. These results convince us that metal diiodides have many benefits for future spintronic devices. |
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ISSN: | 2331-8422 |
DOI: | 10.48550/arxiv.2107.13287 |