Kaixin Zou, Yuxin Yang, Baojuan Xin, Wentao Wu, Yahui Cheng, Hong Dong, Hui Liu, Feng Luo, Feng Lu, Wei-Hua Wang
{"title":"作为潜在二维变磁体和半金属的单层 M2X2O:第一原理研究。","authors":"Kaixin Zou, Yuxin Yang, Baojuan Xin, Wentao Wu, Yahui Cheng, Hong Dong, Hui Liu, Feng Luo, Feng Lu, Wei-Hua Wang","doi":"10.1088/1361-648X/ad8e9f","DOIUrl":null,"url":null,"abstract":"<p><p>Realizing novel two-dimensional (2D) magnetic states would accelerate the development of advanced spintronic devices and the understandings of 2D magnetic physics. In this paper, we have examined the magnetic and electronic properties of 20 dynamically stable and exfoliable M<sub>2</sub>X<sub>2</sub>O (M = Ti-Ni; X = S-Te; excluding Co<sub>2</sub>Te<sub>2</sub>O). It has been unveiled that [X<sub>4</sub>O<sub>2</sub>]-<i>D</i><sub>2<i>h</i></sub>and [M<sub>4</sub>]-<i>D</i><sub>4<i>h</i></sub>crystal fields govern the M-3<i>d</i>orbital splittings in M<sub>2</sub>X<sub>2</sub>O. The splittings further lead to the antiferromagnetic (AFM) orderings in Ti<sub>2</sub>S<sub>2</sub>O/Fe<sub>2</sub>S<sub>2</sub>O/Fe<sub>2</sub>Se<sub>2</sub>O/M<sub>2</sub>X<sub>2</sub>O (M = V, Cr, Mn and Ni; X = S-Se) as well as the ferromagnetic orderings in Ti<sub>2</sub>Se<sub>2</sub>O/Ti<sub>2</sub>Te<sub>2</sub>O/Fe<sub>2</sub>Te<sub>2</sub>O/Co<sub>2</sub>S<sub>2</sub>O/Co<sub>2</sub>Se<sub>2</sub>O through kinetic and superexchange mechanisms. Notably, all the AFM M<sub>2</sub>X<sub>2</sub>O are 2D altermagnets, and Ti<sub>2</sub>Se<sub>2</sub>O/Ti<sub>2</sub>Te<sub>2</sub>O/Co<sub>2</sub>S<sub>2</sub>O/Co<sub>2</sub>Se<sub>2</sub>O are 2D half-metals. In particular, the anisotropic<i>d-d/p</i>hoppings lead to the tunable altermagnetic splitting in Ti<sub>2</sub>S<sub>2</sub>O/Cr<sub>2</sub>Te<sub>2</sub>O, while the parity of V-3<i>d<sub>yz</sub></i>orbital contributes to the symmetry-protected altermagnetic splitting within V<sub>2</sub>X<sub>2</sub>O. These altermagnetic and half-metallic monolayer M<sub>2</sub>X<sub>2</sub>O provide promising candidates applied in low-dimensional spintronic devices. In addition, the potential 2D altermagnetic Weyl semimetal of Fe<sub>2</sub>S<sub>2</sub>O/Fe<sub>2</sub>Se<sub>2</sub>O, nodal-loop half-metal of Ti<sub>2</sub>Se<sub>2</sub>O and half-semi metal of Ti<sub>2</sub>Te<sub>2</sub>O facilitate to uncover novel low-dimensional topological physics. These theoretical results would expand the platform in particular for 2D altermagnets and nontrivial systems.</p>","PeriodicalId":16776,"journal":{"name":"Journal of Physics: Condensed Matter","volume":" ","pages":""},"PeriodicalIF":2.3000,"publicationDate":"2024-11-19","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Monolayer M<sub>2</sub>X<sub>2</sub>O as potential 2D altermagnets and half-metals: a first principles study.\",\"authors\":\"Kaixin Zou, Yuxin Yang, Baojuan Xin, Wentao Wu, Yahui Cheng, Hong Dong, Hui Liu, Feng Luo, Feng Lu, Wei-Hua Wang\",\"doi\":\"10.1088/1361-648X/ad8e9f\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"<p><p>Realizing novel two-dimensional (2D) magnetic states would accelerate the development of advanced spintronic devices and the understandings of 2D magnetic physics. In this paper, we have examined the magnetic and electronic properties of 20 dynamically stable and exfoliable M<sub>2</sub>X<sub>2</sub>O (M = Ti-Ni; X = S-Te; excluding Co<sub>2</sub>Te<sub>2</sub>O). It has been unveiled that [X<sub>4</sub>O<sub>2</sub>]-<i>D</i><sub>2<i>h</i></sub>and [M<sub>4</sub>]-<i>D</i><sub>4<i>h</i></sub>crystal fields govern the M-3<i>d</i>orbital splittings in M<sub>2</sub>X<sub>2</sub>O. The splittings further lead to the antiferromagnetic (AFM) orderings in Ti<sub>2</sub>S<sub>2</sub>O/Fe<sub>2</sub>S<sub>2</sub>O/Fe<sub>2</sub>Se<sub>2</sub>O/M<sub>2</sub>X<sub>2</sub>O (M = V, Cr, Mn and Ni; X = S-Se) as well as the ferromagnetic orderings in Ti<sub>2</sub>Se<sub>2</sub>O/Ti<sub>2</sub>Te<sub>2</sub>O/Fe<sub>2</sub>Te<sub>2</sub>O/Co<sub>2</sub>S<sub>2</sub>O/Co<sub>2</sub>Se<sub>2</sub>O through kinetic and superexchange mechanisms. Notably, all the AFM M<sub>2</sub>X<sub>2</sub>O are 2D altermagnets, and Ti<sub>2</sub>Se<sub>2</sub>O/Ti<sub>2</sub>Te<sub>2</sub>O/Co<sub>2</sub>S<sub>2</sub>O/Co<sub>2</sub>Se<sub>2</sub>O are 2D half-metals. In particular, the anisotropic<i>d-d/p</i>hoppings lead to the tunable altermagnetic splitting in Ti<sub>2</sub>S<sub>2</sub>O/Cr<sub>2</sub>Te<sub>2</sub>O, while the parity of V-3<i>d<sub>yz</sub></i>orbital contributes to the symmetry-protected altermagnetic splitting within V<sub>2</sub>X<sub>2</sub>O. These altermagnetic and half-metallic monolayer M<sub>2</sub>X<sub>2</sub>O provide promising candidates applied in low-dimensional spintronic devices. In addition, the potential 2D altermagnetic Weyl semimetal of Fe<sub>2</sub>S<sub>2</sub>O/Fe<sub>2</sub>Se<sub>2</sub>O, nodal-loop half-metal of Ti<sub>2</sub>Se<sub>2</sub>O and half-semi metal of Ti<sub>2</sub>Te<sub>2</sub>O facilitate to uncover novel low-dimensional topological physics. These theoretical results would expand the platform in particular for 2D altermagnets and nontrivial systems.</p>\",\"PeriodicalId\":16776,\"journal\":{\"name\":\"Journal of Physics: Condensed Matter\",\"volume\":\" \",\"pages\":\"\"},\"PeriodicalIF\":2.3000,\"publicationDate\":\"2024-11-19\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Journal of Physics: Condensed Matter\",\"FirstCategoryId\":\"101\",\"ListUrlMain\":\"https://doi.org/10.1088/1361-648X/ad8e9f\",\"RegionNum\":4,\"RegionCategory\":\"物理与天体物理\",\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"Q3\",\"JCRName\":\"PHYSICS, CONDENSED MATTER\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Journal of Physics: Condensed Matter","FirstCategoryId":"101","ListUrlMain":"https://doi.org/10.1088/1361-648X/ad8e9f","RegionNum":4,"RegionCategory":"物理与天体物理","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q3","JCRName":"PHYSICS, CONDENSED MATTER","Score":null,"Total":0}
Monolayer M2X2O as potential 2D altermagnets and half-metals: a first principles study.
Realizing novel two-dimensional (2D) magnetic states would accelerate the development of advanced spintronic devices and the understandings of 2D magnetic physics. In this paper, we have examined the magnetic and electronic properties of 20 dynamically stable and exfoliable M2X2O (M = Ti-Ni; X = S-Te; excluding Co2Te2O). It has been unveiled that [X4O2]-D2hand [M4]-D4hcrystal fields govern the M-3dorbital splittings in M2X2O. The splittings further lead to the antiferromagnetic (AFM) orderings in Ti2S2O/Fe2S2O/Fe2Se2O/M2X2O (M = V, Cr, Mn and Ni; X = S-Se) as well as the ferromagnetic orderings in Ti2Se2O/Ti2Te2O/Fe2Te2O/Co2S2O/Co2Se2O through kinetic and superexchange mechanisms. Notably, all the AFM M2X2O are 2D altermagnets, and Ti2Se2O/Ti2Te2O/Co2S2O/Co2Se2O are 2D half-metals. In particular, the anisotropicd-d/phoppings lead to the tunable altermagnetic splitting in Ti2S2O/Cr2Te2O, while the parity of V-3dyzorbital contributes to the symmetry-protected altermagnetic splitting within V2X2O. These altermagnetic and half-metallic monolayer M2X2O provide promising candidates applied in low-dimensional spintronic devices. In addition, the potential 2D altermagnetic Weyl semimetal of Fe2S2O/Fe2Se2O, nodal-loop half-metal of Ti2Se2O and half-semi metal of Ti2Te2O facilitate to uncover novel low-dimensional topological physics. These theoretical results would expand the platform in particular for 2D altermagnets and nontrivial systems.
期刊介绍:
Journal of Physics: Condensed Matter covers the whole of condensed matter physics including soft condensed matter and nanostructures. Papers may report experimental, theoretical and simulation studies. Note that papers must contain fundamental condensed matter science: papers reporting methods of materials preparation or properties of materials without novel condensed matter content will not be accepted.