The electronic structure and optical properties of Mn and B, C, N co-doped MoS2 monolayers

The electronic structure and optical properties of Mn and B, C, N co-doped molybdenum disulfide (MoS 2 ) monolayers have been investigated through first-principles calculations. It is shown that the MoS 2 monolayer reflects magnetism with a magnetic moment of 0.87 μB when co-doped with Mn-C. However...

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Veröffentlicht in:Nanoscale research letters 2014-10, Vol.9 (1), p.554-554, Article 554
Hauptverfasser: Xu, Wei-bin, Huang, Bao-jun, Li, Ping, Li, Feng, Zhang, Chang-wen, Wang, Pei-ji
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Li, Feng
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Wang, Pei-ji
description The electronic structure and optical properties of Mn and B, C, N co-doped molybdenum disulfide (MoS 2 ) monolayers have been investigated through first-principles calculations. It is shown that the MoS 2 monolayer reflects magnetism with a magnetic moment of 0.87 μB when co-doped with Mn-C. However, the systems co-doped with Mn-B and Mn-N atoms exhibit semiconducting behavior and their energy bandgaps are 1.03 and 0.81 eV, respectively. The bandgaps of the co-doped systems are smaller than those of the corresponding pristine forms, due to effective charge compensation between Mn and B (N) atoms. The optical properties of Mn-B (C, N) co-doped systems all reflect the redshift phenomenon. The absorption edge of the pure molybdenum disulfide monolayer is 0.8 eV, while the absorption edges of the Mn-B, Mn-C, and Mn-N co-doped systems become 0.45, 0.5, and 0 eV, respectively. As a potential material, MoS 2 is widely used in many fields such as the production of optoelectronic devices, military devices, and civil devices.
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It is shown that the MoS 2 monolayer reflects magnetism with a magnetic moment of 0.87 μB when co-doped with Mn-C. However, the systems co-doped with Mn-B and Mn-N atoms exhibit semiconducting behavior and their energy bandgaps are 1.03 and 0.81 eV, respectively. The bandgaps of the co-doped systems are smaller than those of the corresponding pristine forms, due to effective charge compensation between Mn and B (N) atoms. The optical properties of Mn-B (C, N) co-doped systems all reflect the redshift phenomenon. The absorption edge of the pure molybdenum disulfide monolayer is 0.8 eV, while the absorption edges of the Mn-B, Mn-C, and Mn-N co-doped systems become 0.45, 0.5, and 0 eV, respectively. As a potential material, MoS 2 is widely used in many fields such as the production of optoelectronic devices, military devices, and civil devices.</description><identifier>ISSN: 1931-7573</identifier><identifier>ISSN: 1556-276X</identifier><identifier>EISSN: 1556-276X</identifier><identifier>DOI: 10.1186/1556-276X-9-554</identifier><identifier>PMID: 25317103</identifier><language>eng</language><publisher>New York: Springer New York</publisher><subject>Chemistry and Materials Science ; Materials Science ; Molecular Medicine ; Nano Express ; Nanochemistry ; Nanoscale Science and Technology ; Nanotechnology ; Nanotechnology and Microengineering</subject><ispartof>Nanoscale research letters, 2014-10, Vol.9 (1), p.554-554, Article 554</ispartof><rights>Xu et al.; licensee Springer. 2014. This article is published under license to BioMed Central Ltd. 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It is shown that the MoS 2 monolayer reflects magnetism with a magnetic moment of 0.87 μB when co-doped with Mn-C. However, the systems co-doped with Mn-B and Mn-N atoms exhibit semiconducting behavior and their energy bandgaps are 1.03 and 0.81 eV, respectively. The bandgaps of the co-doped systems are smaller than those of the corresponding pristine forms, due to effective charge compensation between Mn and B (N) atoms. The optical properties of Mn-B (C, N) co-doped systems all reflect the redshift phenomenon. The absorption edge of the pure molybdenum disulfide monolayer is 0.8 eV, while the absorption edges of the Mn-B, Mn-C, and Mn-N co-doped systems become 0.45, 0.5, and 0 eV, respectively. 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It is shown that the MoS 2 monolayer reflects magnetism with a magnetic moment of 0.87 μB when co-doped with Mn-C. However, the systems co-doped with Mn-B and Mn-N atoms exhibit semiconducting behavior and their energy bandgaps are 1.03 and 0.81 eV, respectively. The bandgaps of the co-doped systems are smaller than those of the corresponding pristine forms, due to effective charge compensation between Mn and B (N) atoms. The optical properties of Mn-B (C, N) co-doped systems all reflect the redshift phenomenon. The absorption edge of the pure molybdenum disulfide monolayer is 0.8 eV, while the absorption edges of the Mn-B, Mn-C, and Mn-N co-doped systems become 0.45, 0.5, and 0 eV, respectively. As a potential material, MoS 2 is widely used in many fields such as the production of optoelectronic devices, military devices, and civil devices.</abstract><cop>New York</cop><pub>Springer New York</pub><pmid>25317103</pmid><doi>10.1186/1556-276X-9-554</doi><tpages>1</tpages><oa>free_for_read</oa></addata></record>
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subjects Chemistry and Materials Science
Materials Science
Molecular Medicine
Nano Express
Nanochemistry
Nanoscale Science and Technology
Nanotechnology
Nanotechnology and Microengineering
title The electronic structure and optical properties of Mn and B, C, N co-doped MoS2 monolayers
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