{"title":"WCl3 单层:外加电场下电子和磁性能的第一原理预测","authors":"Md. Azaharuddin Ahmed, A. L. Safi","doi":"10.1007/s10825-024-02195-0","DOIUrl":null,"url":null,"abstract":"<div><p>This current study focuses on predicting the electronic and magnetic behaviors of WCl<sub>3</sub> monolayer when subjected to an external electric field. Unlike CrI<sub>3</sub>, the WCl<sub>3</sub> monolayer displays a preference for an antiferromagnetic (AFM) ground state with an in-plane easy axis. This AFM state remains consistent across the entire spectrum (0–1 V/Å) of the external electric field. The indirect electronic band gap of the WCl<sub>3</sub> monolayer is predicted to be about 2.16 eV. Through our analysis, we’ve identified that the dominance of the valence band maximum and the conduction band minimum stems mainly from the <span>\\({d}_{{x}^{2}-{y}^{2}}\\)</span> orbital (52% contribution) and the <span>\\({d}_{{z}^{2}}\\)</span> orbital (97% contribution) respectively, attributed to the W element. The majority of electronic transitions related to the band gap arise due to these specific orbitals. Furthermore, the application of an external electric field can adjust the band gap to zero, prompting a transition from semiconductor to metal at an electric field intensity of <i>E</i> = 0.9 V/Å. Using mean field theory, we estimate the Neel temperature (<i>T</i><sub>N</sub>) of the AFM system to be approximately 356 K, a notably high value surpassing room temperature. Moreover, the application of an electric field demonstrates the potential to further elevate the Neel temperature, crucial for the functionality of high-temperature spintronic devices. Our comprehensive examination also delves into the magnetic anisotropy of the WCl<sub>3</sub> monolayer. The analysis of magnetic anisotropy energy (MAE) indicates that, contrary to the CrI<sub>3</sub> monolayer, the transition metal W significantly contributes to the system’s MAE, which is predicted to be − <span>\\(3.44\\text{ meV}/\\text{W}\\)</span>. The magnetic easy axis aligns along the <span>\\(x\\)</span> direction (in-plane).</p></div>","PeriodicalId":620,"journal":{"name":"Journal of Computational Electronics","volume":"23 5","pages":"957 - 967"},"PeriodicalIF":2.2000,"publicationDate":"2024-07-06","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"WCl3 monolayer: a first principles prediction of electronic and magnetic properties under an external electric field\",\"authors\":\"Md. Azaharuddin Ahmed, A. L. Safi\",\"doi\":\"10.1007/s10825-024-02195-0\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<div><p>This current study focuses on predicting the electronic and magnetic behaviors of WCl<sub>3</sub> monolayer when subjected to an external electric field. Unlike CrI<sub>3</sub>, the WCl<sub>3</sub> monolayer displays a preference for an antiferromagnetic (AFM) ground state with an in-plane easy axis. This AFM state remains consistent across the entire spectrum (0–1 V/Å) of the external electric field. The indirect electronic band gap of the WCl<sub>3</sub> monolayer is predicted to be about 2.16 eV. Through our analysis, we’ve identified that the dominance of the valence band maximum and the conduction band minimum stems mainly from the <span>\\\\({d}_{{x}^{2}-{y}^{2}}\\\\)</span> orbital (52% contribution) and the <span>\\\\({d}_{{z}^{2}}\\\\)</span> orbital (97% contribution) respectively, attributed to the W element. The majority of electronic transitions related to the band gap arise due to these specific orbitals. Furthermore, the application of an external electric field can adjust the band gap to zero, prompting a transition from semiconductor to metal at an electric field intensity of <i>E</i> = 0.9 V/Å. Using mean field theory, we estimate the Neel temperature (<i>T</i><sub>N</sub>) of the AFM system to be approximately 356 K, a notably high value surpassing room temperature. Moreover, the application of an electric field demonstrates the potential to further elevate the Neel temperature, crucial for the functionality of high-temperature spintronic devices. Our comprehensive examination also delves into the magnetic anisotropy of the WCl<sub>3</sub> monolayer. The analysis of magnetic anisotropy energy (MAE) indicates that, contrary to the CrI<sub>3</sub> monolayer, the transition metal W significantly contributes to the system’s MAE, which is predicted to be − <span>\\\\(3.44\\\\text{ meV}/\\\\text{W}\\\\)</span>. The magnetic easy axis aligns along the <span>\\\\(x\\\\)</span> direction (in-plane).</p></div>\",\"PeriodicalId\":620,\"journal\":{\"name\":\"Journal of Computational Electronics\",\"volume\":\"23 5\",\"pages\":\"957 - 967\"},\"PeriodicalIF\":2.2000,\"publicationDate\":\"2024-07-06\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Computational Electronics\",\"FirstCategoryId\":\"5\",\"ListUrlMain\":\"https://link.springer.com/article/10.1007/s10825-024-02195-0\",\"RegionNum\":4,\"RegionCategory\":\"工程技术\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"ENGINEERING, ELECTRICAL & ELECTRONIC\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Computational Electronics","FirstCategoryId":"5","ListUrlMain":"https://link.springer.com/article/10.1007/s10825-024-02195-0","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
WCl3 monolayer: a first principles prediction of electronic and magnetic properties under an external electric field
This current study focuses on predicting the electronic and magnetic behaviors of WCl3 monolayer when subjected to an external electric field. Unlike CrI3, the WCl3 monolayer displays a preference for an antiferromagnetic (AFM) ground state with an in-plane easy axis. This AFM state remains consistent across the entire spectrum (0–1 V/Å) of the external electric field. The indirect electronic band gap of the WCl3 monolayer is predicted to be about 2.16 eV. Through our analysis, we’ve identified that the dominance of the valence band maximum and the conduction band minimum stems mainly from the \({d}_{{x}^{2}-{y}^{2}}\) orbital (52% contribution) and the \({d}_{{z}^{2}}\) orbital (97% contribution) respectively, attributed to the W element. The majority of electronic transitions related to the band gap arise due to these specific orbitals. Furthermore, the application of an external electric field can adjust the band gap to zero, prompting a transition from semiconductor to metal at an electric field intensity of E = 0.9 V/Å. Using mean field theory, we estimate the Neel temperature (TN) of the AFM system to be approximately 356 K, a notably high value surpassing room temperature. Moreover, the application of an electric field demonstrates the potential to further elevate the Neel temperature, crucial for the functionality of high-temperature spintronic devices. Our comprehensive examination also delves into the magnetic anisotropy of the WCl3 monolayer. The analysis of magnetic anisotropy energy (MAE) indicates that, contrary to the CrI3 monolayer, the transition metal W significantly contributes to the system’s MAE, which is predicted to be − \(3.44\text{ meV}/\text{W}\). The magnetic easy axis aligns along the \(x\) direction (in-plane).
期刊介绍:
he Journal of Computational Electronics brings together research on all aspects of modeling and simulation of modern electronics. This includes optical, electronic, mechanical, and quantum mechanical aspects, as well as research on the underlying mathematical algorithms and computational details. The related areas of energy conversion/storage and of molecular and biological systems, in which the thrust is on the charge transport, electronic, mechanical, and optical properties, are also covered.
In particular, we encourage manuscripts dealing with device simulation; with optical and optoelectronic systems and photonics; with energy storage (e.g. batteries, fuel cells) and harvesting (e.g. photovoltaic), with simulation of circuits, VLSI layout, logic and architecture (based on, for example, CMOS devices, quantum-cellular automata, QBITs, or single-electron transistors); with electromagnetic simulations (such as microwave electronics and components); or with molecular and biological systems. However, in all these cases, the submitted manuscripts should explicitly address the electronic properties of the relevant systems, materials, or devices and/or present novel contributions to the physical models, computational strategies, or numerical algorithms.