{"title":"CrI3/CrGeTe3量子阱结的理论研究","authors":"S. Soliman, M. Salah","doi":"10.21608/ajnsa.2022.150893.1616","DOIUrl":null,"url":null,"abstract":"Electronic structure calculations were conducted for the CrI3/CrGeTe3 junction with different separations ( z ) between the two slabs, CrI3 and CrGeTe3, which provide a means to resolve the magneto-volume spin coupling. The calculations demonstrate that high electron mobility, high frequency, and strongly electronic structure modification are obtained at a specific value for slab separation ( z ). z =0.36238, which is equivalent to the insulating separation of 13.85 Å, is preferable for free-to-move carriers, while the spin wave maximum is at z=18 Å. The moment observed in the DOS of the CrI3 layer supports an increase in the surface field, which, in turn, explains the effectiveness of the CrI 3 layer in tunneling applications. The CrI3 Fermi surface contains small electronic pockets derived from the Cr-3d doubly degenerate state at M. The doubly degenerate effective mass 𝒎 ∗ is approximately constant near the bottom of the nearly free electron band, but the triply 𝒎 ∗ increases somewhat at the inflection point by the Cr-3d magnetic field. Depending on the number of d-electrons, the junctions CoMnI3/CrGeTe3, MoI3/CrGeTe3 and WI3/CrGeTe3 are examined. The comparison between CoMnI3, MoI3 and WI3, and CrI3 ensures that the performance of the CrI3 layer is due to the activity of Cr-3d, which provides a unique opportunity to control the junction properties. The DOS shape of the MoI3 layer demonstrates fairly interesting magnetic properties that are nearly similar to those of the CrI3 layer.","PeriodicalId":8110,"journal":{"name":"Arab Journal of Nuclear Sciences and Applications","volume":" ","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2023-01-26","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Theoretical study on the quantum well junction CrI3 / CrGeTe3\",\"authors\":\"S. Soliman, M. Salah\",\"doi\":\"10.21608/ajnsa.2022.150893.1616\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Electronic structure calculations were conducted for the CrI3/CrGeTe3 junction with different separations ( z ) between the two slabs, CrI3 and CrGeTe3, which provide a means to resolve the magneto-volume spin coupling. The calculations demonstrate that high electron mobility, high frequency, and strongly electronic structure modification are obtained at a specific value for slab separation ( z ). z =0.36238, which is equivalent to the insulating separation of 13.85 Å, is preferable for free-to-move carriers, while the spin wave maximum is at z=18 Å. The moment observed in the DOS of the CrI3 layer supports an increase in the surface field, which, in turn, explains the effectiveness of the CrI 3 layer in tunneling applications. The CrI3 Fermi surface contains small electronic pockets derived from the Cr-3d doubly degenerate state at M. The doubly degenerate effective mass 𝒎 ∗ is approximately constant near the bottom of the nearly free electron band, but the triply 𝒎 ∗ increases somewhat at the inflection point by the Cr-3d magnetic field. Depending on the number of d-electrons, the junctions CoMnI3/CrGeTe3, MoI3/CrGeTe3 and WI3/CrGeTe3 are examined. The comparison between CoMnI3, MoI3 and WI3, and CrI3 ensures that the performance of the CrI3 layer is due to the activity of Cr-3d, which provides a unique opportunity to control the junction properties. The DOS shape of the MoI3 layer demonstrates fairly interesting magnetic properties that are nearly similar to those of the CrI3 layer.\",\"PeriodicalId\":8110,\"journal\":{\"name\":\"Arab Journal of Nuclear Sciences and Applications\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2023-01-26\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Arab Journal of Nuclear Sciences and Applications\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.21608/ajnsa.2022.150893.1616\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Arab Journal of Nuclear Sciences and Applications","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.21608/ajnsa.2022.150893.1616","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Theoretical study on the quantum well junction CrI3 / CrGeTe3
Electronic structure calculations were conducted for the CrI3/CrGeTe3 junction with different separations ( z ) between the two slabs, CrI3 and CrGeTe3, which provide a means to resolve the magneto-volume spin coupling. The calculations demonstrate that high electron mobility, high frequency, and strongly electronic structure modification are obtained at a specific value for slab separation ( z ). z =0.36238, which is equivalent to the insulating separation of 13.85 Å, is preferable for free-to-move carriers, while the spin wave maximum is at z=18 Å. The moment observed in the DOS of the CrI3 layer supports an increase in the surface field, which, in turn, explains the effectiveness of the CrI 3 layer in tunneling applications. The CrI3 Fermi surface contains small electronic pockets derived from the Cr-3d doubly degenerate state at M. The doubly degenerate effective mass 𝒎 ∗ is approximately constant near the bottom of the nearly free electron band, but the triply 𝒎 ∗ increases somewhat at the inflection point by the Cr-3d magnetic field. Depending on the number of d-electrons, the junctions CoMnI3/CrGeTe3, MoI3/CrGeTe3 and WI3/CrGeTe3 are examined. The comparison between CoMnI3, MoI3 and WI3, and CrI3 ensures that the performance of the CrI3 layer is due to the activity of Cr-3d, which provides a unique opportunity to control the junction properties. The DOS shape of the MoI3 layer demonstrates fairly interesting magnetic properties that are nearly similar to those of the CrI3 layer.