Newtype single-layer magnetic semiconductor in transition-metal dichalcogenides VX2 (X = S, Se and Te)
We present a newtype 2-dimensional (2D) magnetic semiconductor based on transition-metal dichalcogenides VX 2 (X = S, Se and Te) via first-principles calculations. The obtained indirect band gaps of monolayer VS 2 , VSe 2 , and VTe 2 given from the generalized gradient approximation (GGA) are respec...
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description | We present a newtype 2-dimensional (2D) magnetic semiconductor based on transition-metal dichalcogenides VX
2
(X = S, Se and Te) via first-principles calculations. The obtained indirect band gaps of monolayer VS
2
, VSe
2
, and VTe
2
given from the generalized gradient approximation (GGA) are respectively 0.05, 0.22, and 0.20 eV, all with integer magnetic moments of 1.0
μ
B
. The GGA plus on-site Coulomb interaction
U
(GGA +
U
) enhances the exchange splittings and raises the energy gap up to 0.38~0.65 eV. By adopting the GW approximation, we obtain converged G0W0 gaps of 1.3, 1.2, and 0.7 eV for VS
2
, VSe
2
, and VTe
2
monolayers, respectively. They agree very well with our calculated HSE gaps of 1.1, 1.2, and 0.6 eV, respectively. The gap sizes as well as the metal-insulator transitions are tunable by applying the in-plane strain and/or changing the number of stacking layers. The Monte Carlo simulations illustrate very high Curie-temperatures of 292, 472, and 553 K for VS
2
, VSe
2
, and VTe
2
monolayers, respectively. They are nearly or well beyond the room temperature. Combining the semiconducting energy gap, the 100% spin polarized valence and conduction bands, the room temperature T
C
, and the in-plane magnetic anisotropy together in a single layer VX
2
, this newtype 2D magnetic semiconductor shows great potential in future spintronics. |
doi_str_mv | 10.1038/srep32625 |
format | Article |
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2
(X = S, Se and Te) via first-principles calculations. The obtained indirect band gaps of monolayer VS
2
, VSe
2
, and VTe
2
given from the generalized gradient approximation (GGA) are respectively 0.05, 0.22, and 0.20 eV, all with integer magnetic moments of 1.0
μ
B
. The GGA plus on-site Coulomb interaction
U
(GGA +
U
) enhances the exchange splittings and raises the energy gap up to 0.38~0.65 eV. By adopting the GW approximation, we obtain converged G0W0 gaps of 1.3, 1.2, and 0.7 eV for VS
2
, VSe
2
, and VTe
2
monolayers, respectively. They agree very well with our calculated HSE gaps of 1.1, 1.2, and 0.6 eV, respectively. The gap sizes as well as the metal-insulator transitions are tunable by applying the in-plane strain and/or changing the number of stacking layers. The Monte Carlo simulations illustrate very high Curie-temperatures of 292, 472, and 553 K for VS
2
, VSe
2
, and VTe
2
monolayers, respectively. They are nearly or well beyond the room temperature. Combining the semiconducting energy gap, the 100% spin polarized valence and conduction bands, the room temperature T
C
, and the in-plane magnetic anisotropy together in a single layer VX
2
, this newtype 2D magnetic semiconductor shows great potential in future spintronics.</description><identifier>ISSN: 2045-2322</identifier><identifier>EISSN: 2045-2322</identifier><identifier>DOI: 10.1038/srep32625</identifier><identifier>PMID: 27601195</identifier><language>eng</language><publisher>London: Nature Publishing Group UK</publisher><subject>639/301/119/2793 ; 639/301/357/1018 ; 639/766/119/1001 ; 639/766/119/997 ; Conduction ; Energy ; Humanities and Social Sciences ; Monte Carlo simulation ; multidisciplinary ; Science ; Temperature effects</subject><ispartof>Scientific reports, 2016-09, Vol.6 (1), p.32625-32625, Article 32625</ispartof><rights>The Author(s) 2016</rights><rights>Copyright Nature Publishing Group Sep 2016</rights><rights>Copyright © 2016, The Author(s) 2016 The Author(s)</rights><lds50>peer_reviewed</lds50><oa>free_for_read</oa><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c368t-8d7afbc8d94c4e00941b25bb23dc34a19f4aa4b0d19ed3b59eb561838f79af563</citedby><cites>FETCH-LOGICAL-c368t-8d7afbc8d94c4e00941b25bb23dc34a19f4aa4b0d19ed3b59eb561838f79af563</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.ncbi.nlm.nih.gov/pmc/articles/PMC5013522/pdf/$$EPDF$$P50$$Gpubmedcentral$$Hfree_for_read</linktopdf><linktohtml>$$Uhttps://www.ncbi.nlm.nih.gov/pmc/articles/PMC5013522/$$EHTML$$P50$$Gpubmedcentral$$Hfree_for_read</linktohtml><link.rule.ids>230,315,729,782,786,866,887,27931,27932,41127,42196,51583,53798,53800</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/27601195$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Fuh, Huei-Ru</creatorcontrib><creatorcontrib>Chang, Ching-Ray</creatorcontrib><creatorcontrib>Wang, Yin-Kuo</creatorcontrib><creatorcontrib>Evans, Richard F. L.</creatorcontrib><creatorcontrib>Chantrell, Roy W.</creatorcontrib><creatorcontrib>Jeng, Horng-Tay</creatorcontrib><title>Newtype single-layer magnetic semiconductor in transition-metal dichalcogenides VX2 (X = S, Se and Te)</title><title>Scientific reports</title><addtitle>Sci Rep</addtitle><addtitle>Sci Rep</addtitle><description>We present a newtype 2-dimensional (2D) magnetic semiconductor based on transition-metal dichalcogenides VX
2
(X = S, Se and Te) via first-principles calculations. The obtained indirect band gaps of monolayer VS
2
, VSe
2
, and VTe
2
given from the generalized gradient approximation (GGA) are respectively 0.05, 0.22, and 0.20 eV, all with integer magnetic moments of 1.0
μ
B
. The GGA plus on-site Coulomb interaction
U
(GGA +
U
) enhances the exchange splittings and raises the energy gap up to 0.38~0.65 eV. By adopting the GW approximation, we obtain converged G0W0 gaps of 1.3, 1.2, and 0.7 eV for VS
2
, VSe
2
, and VTe
2
monolayers, respectively. They agree very well with our calculated HSE gaps of 1.1, 1.2, and 0.6 eV, respectively. The gap sizes as well as the metal-insulator transitions are tunable by applying the in-plane strain and/or changing the number of stacking layers. The Monte Carlo simulations illustrate very high Curie-temperatures of 292, 472, and 553 K for VS
2
, VSe
2
, and VTe
2
monolayers, respectively. They are nearly or well beyond the room temperature. Combining the semiconducting energy gap, the 100% spin polarized valence and conduction bands, the room temperature T
C
, and the in-plane magnetic anisotropy together in a single layer VX
2
, this newtype 2D magnetic semiconductor shows great potential in future spintronics.</description><subject>639/301/119/2793</subject><subject>639/301/357/1018</subject><subject>639/766/119/1001</subject><subject>639/766/119/997</subject><subject>Conduction</subject><subject>Energy</subject><subject>Humanities and Social Sciences</subject><subject>Monte Carlo simulation</subject><subject>multidisciplinary</subject><subject>Science</subject><subject>Temperature effects</subject><issn>2045-2322</issn><issn>2045-2322</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2016</creationdate><recordtype>article</recordtype><sourceid>C6C</sourceid><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GNUQQ</sourceid><recordid>eNplkU9rFTEUxYMotrRd-AUk4KYVR_NnMpMsFKSoFYouWqW7kEnuTPOYSZ7JjPJ2bv2afhIjrz6eeiHcwPlxcsJB6BElzynh8kVOsOasYeIeOmSkFhXjjN3fux-gk5xXpIxgqqbqITpgbUMoVeIQrT7At3mzBpx9GEaoRrOBhCczBJi9xRkmb2Nwi51jwj7gOZmQ_exjqCaYzYidt7dmtHGA4B1k_PmG4dObn99_vCzn6hm-AmyCw9dwdowe9GbMcHK3j9Cnt2-uzy-qy4_v3p-_vqwsb-RcSdeavrPSqdrWQEiJ3DHRdYw7y2tDVV8bU3fEUQWOd0JBJxoquexbZXrR8CP0auu7XroJnIVQQo96nfxk0kZH4_XfSvC3eohftSCUC8aKwemdQYpfFsiznny2MI4mQFyyppK2kjWk5QV98g-6iksK5XuFUoo0SklZqLMtZVPMpa9-F4YS_btEvSuxsI_30-_IP5UV4OkWyEUKA6S9J_9z-wUMtqh4</recordid><startdate>20160907</startdate><enddate>20160907</enddate><creator>Fuh, Huei-Ru</creator><creator>Chang, Ching-Ray</creator><creator>Wang, Yin-Kuo</creator><creator>Evans, Richard F. 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L. ; Chantrell, Roy W. ; Jeng, Horng-Tay</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c368t-8d7afbc8d94c4e00941b25bb23dc34a19f4aa4b0d19ed3b59eb561838f79af563</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2016</creationdate><topic>639/301/119/2793</topic><topic>639/301/357/1018</topic><topic>639/766/119/1001</topic><topic>639/766/119/997</topic><topic>Conduction</topic><topic>Energy</topic><topic>Humanities and Social Sciences</topic><topic>Monte Carlo simulation</topic><topic>multidisciplinary</topic><topic>Science</topic><topic>Temperature effects</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Fuh, Huei-Ru</creatorcontrib><creatorcontrib>Chang, Ching-Ray</creatorcontrib><creatorcontrib>Wang, Yin-Kuo</creatorcontrib><creatorcontrib>Evans, Richard F. L.</creatorcontrib><creatorcontrib>Chantrell, Roy W.</creatorcontrib><creatorcontrib>Jeng, Horng-Tay</creatorcontrib><collection>Springer Nature OA/Free Journals</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>ProQuest Central (Corporate)</collection><collection>Health & Medical Collection</collection><collection>ProQuest Central (purchase pre-March 2016)</collection><collection>Biology Database (Alumni Edition)</collection><collection>Medical Database (Alumni Edition)</collection><collection>Science Database (Alumni Edition)</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Natural Science Collection</collection><collection>Hospital Premium Collection</collection><collection>Hospital Premium Collection (Alumni Edition)</collection><collection>ProQuest Central (Alumni) (purchase pre-March 2016)</collection><collection>ProQuest Central (Alumni Edition)</collection><collection>ProQuest Central UK/Ireland</collection><collection>ProQuest Central Essentials</collection><collection>Biological Science Collection</collection><collection>ProQuest Central</collection><collection>Natural Science Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Central Korea</collection><collection>Health Research Premium Collection</collection><collection>Health Research Premium Collection (Alumni)</collection><collection>ProQuest Central Student</collection><collection>SciTech Premium Collection</collection><collection>ProQuest Health & Medical Complete (Alumni)</collection><collection>ProQuest Biological Science Collection</collection><collection>Health & Medical Collection (Alumni Edition)</collection><collection>Medical Database</collection><collection>Science Database</collection><collection>Biological Science Database</collection><collection>Access via ProQuest (Open Access)</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>ProQuest Central Basic</collection><collection>MEDLINE - Academic</collection><collection>PubMed Central (Full Participant titles)</collection><jtitle>Scientific reports</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Fuh, Huei-Ru</au><au>Chang, Ching-Ray</au><au>Wang, Yin-Kuo</au><au>Evans, Richard F. L.</au><au>Chantrell, Roy W.</au><au>Jeng, Horng-Tay</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Newtype single-layer magnetic semiconductor in transition-metal dichalcogenides VX2 (X = S, Se and Te)</atitle><jtitle>Scientific reports</jtitle><stitle>Sci Rep</stitle><addtitle>Sci Rep</addtitle><date>2016-09-07</date><risdate>2016</risdate><volume>6</volume><issue>1</issue><spage>32625</spage><epage>32625</epage><pages>32625-32625</pages><artnum>32625</artnum><issn>2045-2322</issn><eissn>2045-2322</eissn><abstract>We present a newtype 2-dimensional (2D) magnetic semiconductor based on transition-metal dichalcogenides VX
2
(X = S, Se and Te) via first-principles calculations. The obtained indirect band gaps of monolayer VS
2
, VSe
2
, and VTe
2
given from the generalized gradient approximation (GGA) are respectively 0.05, 0.22, and 0.20 eV, all with integer magnetic moments of 1.0
μ
B
. The GGA plus on-site Coulomb interaction
U
(GGA +
U
) enhances the exchange splittings and raises the energy gap up to 0.38~0.65 eV. By adopting the GW approximation, we obtain converged G0W0 gaps of 1.3, 1.2, and 0.7 eV for VS
2
, VSe
2
, and VTe
2
monolayers, respectively. They agree very well with our calculated HSE gaps of 1.1, 1.2, and 0.6 eV, respectively. The gap sizes as well as the metal-insulator transitions are tunable by applying the in-plane strain and/or changing the number of stacking layers. The Monte Carlo simulations illustrate very high Curie-temperatures of 292, 472, and 553 K for VS
2
, VSe
2
, and VTe
2
monolayers, respectively. They are nearly or well beyond the room temperature. Combining the semiconducting energy gap, the 100% spin polarized valence and conduction bands, the room temperature T
C
, and the in-plane magnetic anisotropy together in a single layer VX
2
, this newtype 2D magnetic semiconductor shows great potential in future spintronics.</abstract><cop>London</cop><pub>Nature Publishing Group UK</pub><pmid>27601195</pmid><doi>10.1038/srep32625</doi><tpages>1</tpages><oa>free_for_read</oa></addata></record> |
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subjects | 639/301/119/2793 639/301/357/1018 639/766/119/1001 639/766/119/997 Conduction Energy Humanities and Social Sciences Monte Carlo simulation multidisciplinary Science Temperature effects |
title | Newtype single-layer magnetic semiconductor in transition-metal dichalcogenides VX2 (X = S, Se and Te) |
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