Valley polarization and magnetic anisotropy of two-dimensional Ni 2 Cl 3 I 3 /MoSe 2 heterostructures
Two-dimensional (2D) Janus trihalides have attracted widespread attention due to their potential applications in spintronics. In this work, the valley polarization of MoSe at the K' and K points can be modulated by Ni Cl I , a new 2D Janus trihalide. The Ni Cl I /MoSe heterostructure has an in-...
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Veröffentlicht in: | Nanoscale 2024-06, Vol.16 (25), p.12196-12206 |
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description | Two-dimensional (2D) Janus trihalides have attracted widespread attention due to their potential applications in spintronics. In this work, the valley polarization of MoSe
at the K' and K points can be modulated by Ni
Cl
I
, a new 2D Janus trihalide. The Ni
Cl
I
/MoSe
heterostructure has an in-plane magnetic anisotropy energy (IMA) and is characterized by three distinct electronic structures: metallic, semiconducting, and half-metallic. It is noted that the semiconducting state features a band gap of 0.07 eV. When spin-orbit coupling (SOC) is considered, valley polarization is exhibited in the Ni
Cl
I
/MoSe
heterostructure, with the degree of valley polarization varying across different configurations and reaching a maximum value of 4.6 meV. The electronic properties, valley polarization and MAE of the system can be tuned by biaxial strains. The application of a biaxial strain ranging from -6% to +6% can enhance the valley polarization value from 0.9 meV to 12.9 meV. The directions of MAE of the Ni
Cl
I
/MoSe
heterostructure can be changed at biaxial strains of -6%, +2%, +4% and +6%. The above calculation results show that the heterostructure system possesses rich electronic properties and tunability, with extensive potential applications in the fields of spintronic and valleytronic devices. |
doi_str_mv | 10.1039/d4nr01253d |
format | Article |
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at the K' and K points can be modulated by Ni
Cl
I
, a new 2D Janus trihalide. The Ni
Cl
I
/MoSe
heterostructure has an in-plane magnetic anisotropy energy (IMA) and is characterized by three distinct electronic structures: metallic, semiconducting, and half-metallic. It is noted that the semiconducting state features a band gap of 0.07 eV. When spin-orbit coupling (SOC) is considered, valley polarization is exhibited in the Ni
Cl
I
/MoSe
heterostructure, with the degree of valley polarization varying across different configurations and reaching a maximum value of 4.6 meV. The electronic properties, valley polarization and MAE of the system can be tuned by biaxial strains. The application of a biaxial strain ranging from -6% to +6% can enhance the valley polarization value from 0.9 meV to 12.9 meV. The directions of MAE of the Ni
Cl
I
/MoSe
heterostructure can be changed at biaxial strains of -6%, +2%, +4% and +6%. The above calculation results show that the heterostructure system possesses rich electronic properties and tunability, with extensive potential applications in the fields of spintronic and valleytronic devices.</description><identifier>ISSN: 2040-3364</identifier><identifier>EISSN: 2040-3372</identifier><identifier>DOI: 10.1039/d4nr01253d</identifier><identifier>PMID: 38842385</identifier><language>eng</language><publisher>England</publisher><ispartof>Nanoscale, 2024-06, Vol.16 (25), p.12196-12206</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c585-16fa3ed37b2806bcc5435ecf8bbe1b651b3dc301e2431275fb851fbac8d76b0f3</cites><orcidid>0000-0002-3467-4594 ; 0000-0003-3568-701X</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27901,27902</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/38842385$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Chen, Bo</creatorcontrib><creatorcontrib>Zhou, Baozeng</creatorcontrib><creatorcontrib>Wang, Xiaocha</creatorcontrib><title>Valley polarization and magnetic anisotropy of two-dimensional Ni 2 Cl 3 I 3 /MoSe 2 heterostructures</title><title>Nanoscale</title><addtitle>Nanoscale</addtitle><description>Two-dimensional (2D) Janus trihalides have attracted widespread attention due to their potential applications in spintronics. In this work, the valley polarization of MoSe
at the K' and K points can be modulated by Ni
Cl
I
, a new 2D Janus trihalide. The Ni
Cl
I
/MoSe
heterostructure has an in-plane magnetic anisotropy energy (IMA) and is characterized by three distinct electronic structures: metallic, semiconducting, and half-metallic. It is noted that the semiconducting state features a band gap of 0.07 eV. When spin-orbit coupling (SOC) is considered, valley polarization is exhibited in the Ni
Cl
I
/MoSe
heterostructure, with the degree of valley polarization varying across different configurations and reaching a maximum value of 4.6 meV. The electronic properties, valley polarization and MAE of the system can be tuned by biaxial strains. The application of a biaxial strain ranging from -6% to +6% can enhance the valley polarization value from 0.9 meV to 12.9 meV. The directions of MAE of the Ni
Cl
I
/MoSe
heterostructure can be changed at biaxial strains of -6%, +2%, +4% and +6%. The above calculation results show that the heterostructure system possesses rich electronic properties and tunability, with extensive potential applications in the fields of spintronic and valleytronic devices.</description><issn>2040-3364</issn><issn>2040-3372</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2024</creationdate><recordtype>article</recordtype><recordid>eNo9kNtKAzEQhoMotlZvfADJtbA2yWx200tpPRRqBS3eLjnqyu5mSVKkPr3rqRfDzD98zMCH0DklV5TAbGryLhDKOJgDNGYkJxlAyQ73c5GP0EmM74QUMyjgGI1AiJyB4GNkX2TT2B3ufSND_SlT7TssO4Nb-drZVOsh1NGn4Psd9g6nD5-ZurVdHEDZ4HWNGZ43GPByqOmDf7bD4s0mG3xMYavTNth4io6cbKI9--sTtLm92czvs9Xj3XJ-vco0FzyjhZNgDZSKCVIorXkO3GonlLJUFZwqMBoItSwHykrulODUKamFKQtFHEzQ5e9ZPTyPwbqqD3Urw66ipPpWVS3y9dOPqsUAX_zC_Va11uzRfzfwBdcjZGY</recordid><startdate>20240627</startdate><enddate>20240627</enddate><creator>Chen, Bo</creator><creator>Zhou, Baozeng</creator><creator>Wang, Xiaocha</creator><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-3467-4594</orcidid><orcidid>https://orcid.org/0000-0003-3568-701X</orcidid></search><sort><creationdate>20240627</creationdate><title>Valley polarization and magnetic anisotropy of two-dimensional Ni 2 Cl 3 I 3 /MoSe 2 heterostructures</title><author>Chen, Bo ; Zhou, Baozeng ; Wang, Xiaocha</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c585-16fa3ed37b2806bcc5435ecf8bbe1b651b3dc301e2431275fb851fbac8d76b0f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2024</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chen, Bo</creatorcontrib><creatorcontrib>Zhou, Baozeng</creatorcontrib><creatorcontrib>Wang, Xiaocha</creatorcontrib><collection>PubMed</collection><collection>CrossRef</collection><jtitle>Nanoscale</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Chen, Bo</au><au>Zhou, Baozeng</au><au>Wang, Xiaocha</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Valley polarization and magnetic anisotropy of two-dimensional Ni 2 Cl 3 I 3 /MoSe 2 heterostructures</atitle><jtitle>Nanoscale</jtitle><addtitle>Nanoscale</addtitle><date>2024-06-27</date><risdate>2024</risdate><volume>16</volume><issue>25</issue><spage>12196</spage><epage>12206</epage><pages>12196-12206</pages><issn>2040-3364</issn><eissn>2040-3372</eissn><abstract>Two-dimensional (2D) Janus trihalides have attracted widespread attention due to their potential applications in spintronics. In this work, the valley polarization of MoSe
at the K' and K points can be modulated by Ni
Cl
I
, a new 2D Janus trihalide. The Ni
Cl
I
/MoSe
heterostructure has an in-plane magnetic anisotropy energy (IMA) and is characterized by three distinct electronic structures: metallic, semiconducting, and half-metallic. It is noted that the semiconducting state features a band gap of 0.07 eV. When spin-orbit coupling (SOC) is considered, valley polarization is exhibited in the Ni
Cl
I
/MoSe
heterostructure, with the degree of valley polarization varying across different configurations and reaching a maximum value of 4.6 meV. The electronic properties, valley polarization and MAE of the system can be tuned by biaxial strains. The application of a biaxial strain ranging from -6% to +6% can enhance the valley polarization value from 0.9 meV to 12.9 meV. The directions of MAE of the Ni
Cl
I
/MoSe
heterostructure can be changed at biaxial strains of -6%, +2%, +4% and +6%. The above calculation results show that the heterostructure system possesses rich electronic properties and tunability, with extensive potential applications in the fields of spintronic and valleytronic devices.</abstract><cop>England</cop><pmid>38842385</pmid><doi>10.1039/d4nr01253d</doi><tpages>11</tpages><orcidid>https://orcid.org/0000-0002-3467-4594</orcidid><orcidid>https://orcid.org/0000-0003-3568-701X</orcidid></addata></record> |
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source | Royal Society Of Chemistry Journals 2008- |
title | Valley polarization and magnetic anisotropy of two-dimensional Ni 2 Cl 3 I 3 /MoSe 2 heterostructures |
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