Nguyen Thanh Tien, J. Guerrero-Sanchez and D. M. Hoat
{"title":"A systematic study of TMOn (TM = V, Cr, Mn, and Fe; n = 3 and 6) clusters embedded in a PtS2 monolayer†","authors":"Nguyen Thanh Tien, J. Guerrero-Sanchez and D. M. Hoat","doi":"10.1039/D4NA00465E","DOIUrl":null,"url":null,"abstract":"<p >Doping-based magnetism engineering is an effective approach to synthesize new multifunctional two-dimensional (2D) materials from their non-magnetic counterparts. In this work, doping with TMO<small><sub><em>n</em></sub></small> clusters (TM = V, Cr, Mn, and Fe; <em>n</em> = 3 and 6) is proposed to induce feature-rich electronic and magnetic properties in a PtS<small><sub>2</sub></small> monolayer. The pristine monolayer is a non-magnetic semiconductor with an indirect energy gap of 1.81 (2.67) eV as obtained from PBE(HSE06)-based calculations. PtS<small><sub>3</sub></small>-type multivacancies magnetize significantly the monolayer, inducing the emergence of half-metallicity. In this case, a total magnetic moment of 1.90 μ<small><sub>B</sub></small> is obtained and magnetic properties are produced mainly by atoms around the vacancy sites. Meanwhile, the PtS<small><sub>2</sub></small> monolayer is metallized by creating PtS<small><sub>6</sub></small>-type multivacancies without magnetization. Depending on the type of TMO<small><sub><em>n</em></sub></small> cluster, either a feature-rich diluted magnetic semiconductor or half-metallic nature is induced, which is regulated mainly by the incorporated clusters. Except for the FeO<small><sub>6</sub></small> cluster, TM atoms and O atoms exhibit an antiparallel spin orientation, resulting in total magnetic moments between 1.00 and 4.00 μ<small><sub>B</sub></small>. Meanwhile, the parallel spin ordering gives a large total magnetic moment of 5.99 μ<small><sub>B</sub></small> for the FeO<small><sub>6</sub></small>-doped monolayer. Furthermore, Bader charge analysis indicates that all the clusters attract charge from the host monolayer that is mainly due to the electronegative O atoms. Our results may introduce cluster doping as an efficient way to create new spintronic 2D materials from a non-magnetic PtS<small><sub>2</sub></small> monolayer.</p>","PeriodicalId":18806,"journal":{"name":"Nanoscale Advances","volume":null,"pages":null},"PeriodicalIF":4.6000,"publicationDate":"2024-09-10","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://pubs.rsc.org/en/content/articlepdf/2024/na/d4na00465e?page=search","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Nanoscale Advances","FirstCategoryId":"88","ListUrlMain":"https://pubs.rsc.org/en/content/articlelanding/2024/na/d4na00465e","RegionNum":3,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"CHEMISTRY, MULTIDISCIPLINARY","Score":null,"Total":0}
引用次数: 0
Abstract
Doping-based magnetism engineering is an effective approach to synthesize new multifunctional two-dimensional (2D) materials from their non-magnetic counterparts. In this work, doping with TMOn clusters (TM = V, Cr, Mn, and Fe; n = 3 and 6) is proposed to induce feature-rich electronic and magnetic properties in a PtS2 monolayer. The pristine monolayer is a non-magnetic semiconductor with an indirect energy gap of 1.81 (2.67) eV as obtained from PBE(HSE06)-based calculations. PtS3-type multivacancies magnetize significantly the monolayer, inducing the emergence of half-metallicity. In this case, a total magnetic moment of 1.90 μB is obtained and magnetic properties are produced mainly by atoms around the vacancy sites. Meanwhile, the PtS2 monolayer is metallized by creating PtS6-type multivacancies without magnetization. Depending on the type of TMOn cluster, either a feature-rich diluted magnetic semiconductor or half-metallic nature is induced, which is regulated mainly by the incorporated clusters. Except for the FeO6 cluster, TM atoms and O atoms exhibit an antiparallel spin orientation, resulting in total magnetic moments between 1.00 and 4.00 μB. Meanwhile, the parallel spin ordering gives a large total magnetic moment of 5.99 μB for the FeO6-doped monolayer. Furthermore, Bader charge analysis indicates that all the clusters attract charge from the host monolayer that is mainly due to the electronegative O atoms. Our results may introduce cluster doping as an efficient way to create new spintronic 2D materials from a non-magnetic PtS2 monolayer.