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Role of Main Group Nonmetal Dopants on the Electronic Properties of the TcS2 Monolayer Revealed by Density Functional Theory
The electronic properties of n - and p -type semiconductors using nonmetals (H, B, C, N, O, Si, P, Se, F, Cl, Br, and I) to substitute sulfur in the TcS 2 monolayer were investigated using first-principles methods based on the density functional theory. The H-, B-, C-, N-, Si-, and P-doped systems w...
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Published in: | Journal of electronic materials 2023-09, Vol.52 (9), p.5931-5945 |
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creator | Widya Marlina, Lala Adetia Hutama, Aulia Sukma Prasetyo, Niko |
description | The electronic properties of
n
- and
p
-type semiconductors using nonmetals (H, B, C, N, O, Si, P, Se, F, Cl, Br, and I) to substitute sulfur in the TcS
2
monolayer were investigated using first-principles methods based on the density functional theory. The H-, B-, C-, N-, Si-, and P-doped systems were
p
-type, whereas the F-doped systems were
n
-type semiconductors. Numerical results showed that these nonmetals induced magnetic properties through the dopant
p
orbital and neighboring Tc atom
d
orbitals. H-, B-, N-, P-, and F-doped systems exhibited semiconducting magnetic nanomaterial features, whereas Cl-, Br-, and I-doped systems exhibited half-metallic magnetic features. The formation energy of the C-doped system was the lowest followed by the O-doped system, compared to that of the other examined systems. Under Tc-rich growth conditions, the preparation of nonmetal-doped TcS
2
was facile and stable because of its negative impurity formation energy. A more significant change was observed at the band edges of the doped systems compared to the pristine TcS
2
monolayer. These results provided fundamental insights into the doped TcS
2
monolayer for application as photocatalysts and spintronic, optoelectronic, and electronic devices. |
doi_str_mv | 10.1007/s11664-023-10513-8 |
format | article |
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n
- and
p
-type semiconductors using nonmetals (H, B, C, N, O, Si, P, Se, F, Cl, Br, and I) to substitute sulfur in the TcS
2
monolayer were investigated using first-principles methods based on the density functional theory. The H-, B-, C-, N-, Si-, and P-doped systems were
p
-type, whereas the F-doped systems were
n
-type semiconductors. Numerical results showed that these nonmetals induced magnetic properties through the dopant
p
orbital and neighboring Tc atom
d
orbitals. H-, B-, N-, P-, and F-doped systems exhibited semiconducting magnetic nanomaterial features, whereas Cl-, Br-, and I-doped systems exhibited half-metallic magnetic features. The formation energy of the C-doped system was the lowest followed by the O-doped system, compared to that of the other examined systems. Under Tc-rich growth conditions, the preparation of nonmetal-doped TcS
2
was facile and stable because of its negative impurity formation energy. A more significant change was observed at the band edges of the doped systems compared to the pristine TcS
2
monolayer. These results provided fundamental insights into the doped TcS
2
monolayer for application as photocatalysts and spintronic, optoelectronic, and electronic devices.</description><identifier>ISSN: 0361-5235</identifier><identifier>EISSN: 1543-186X</identifier><identifier>DOI: 10.1007/s11664-023-10513-8</identifier><language>eng</language><publisher>New York: Springer US</publisher><subject>Characterization and Evaluation of Materials ; Chemistry and Materials Science ; Density functional theory ; Dopants ; Electronics and Microelectronics ; Energy of formation ; First principles ; Free energy ; Heat of formation ; Instrumentation ; Magnetic properties ; Materials Science ; Monolayers ; N-type semiconductors ; Nanomaterials ; Nonmetals ; Optical and Electronic Materials ; Optoelectronic devices ; Original Research Article ; P-type semiconductors ; Semiconductors ; Solid State Physics</subject><ispartof>Journal of electronic materials, 2023-09, Vol.52 (9), p.5931-5945</ispartof><rights>The Minerals, Metals & Materials Society 2023. Springer Nature or its licensor (e.g. a society or other partner) holds exclusive rights to this article under a publishing agreement with the author(s) or other rightsholder(s); author self-archiving of the accepted manuscript version of this article is solely governed by the terms of such publishing agreement and applicable law.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c270t-9fcf6282fb8417fbb1625c68e20b256ecff0a4b0dd306707afbb99854d944ecc3</cites><orcidid>0000-0002-3322-9421</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Widya</creatorcontrib><creatorcontrib>Marlina, Lala Adetia</creatorcontrib><creatorcontrib>Hutama, Aulia Sukma</creatorcontrib><creatorcontrib>Prasetyo, Niko</creatorcontrib><title>Role of Main Group Nonmetal Dopants on the Electronic Properties of the TcS2 Monolayer Revealed by Density Functional Theory</title><title>Journal of electronic materials</title><addtitle>J. Electron. Mater</addtitle><description>The electronic properties of
n
- and
p
-type semiconductors using nonmetals (H, B, C, N, O, Si, P, Se, F, Cl, Br, and I) to substitute sulfur in the TcS
2
monolayer were investigated using first-principles methods based on the density functional theory. The H-, B-, C-, N-, Si-, and P-doped systems were
p
-type, whereas the F-doped systems were
n
-type semiconductors. Numerical results showed that these nonmetals induced magnetic properties through the dopant
p
orbital and neighboring Tc atom
d
orbitals. H-, B-, N-, P-, and F-doped systems exhibited semiconducting magnetic nanomaterial features, whereas Cl-, Br-, and I-doped systems exhibited half-metallic magnetic features. The formation energy of the C-doped system was the lowest followed by the O-doped system, compared to that of the other examined systems. Under Tc-rich growth conditions, the preparation of nonmetal-doped TcS
2
was facile and stable because of its negative impurity formation energy. A more significant change was observed at the band edges of the doped systems compared to the pristine TcS
2
monolayer. These results provided fundamental insights into the doped TcS
2
monolayer for application as photocatalysts and spintronic, optoelectronic, and electronic devices.</description><subject>Characterization and Evaluation of Materials</subject><subject>Chemistry and Materials Science</subject><subject>Density functional theory</subject><subject>Dopants</subject><subject>Electronics and Microelectronics</subject><subject>Energy of formation</subject><subject>First principles</subject><subject>Free energy</subject><subject>Heat of formation</subject><subject>Instrumentation</subject><subject>Magnetic properties</subject><subject>Materials Science</subject><subject>Monolayers</subject><subject>N-type semiconductors</subject><subject>Nanomaterials</subject><subject>Nonmetals</subject><subject>Optical and Electronic Materials</subject><subject>Optoelectronic devices</subject><subject>Original Research Article</subject><subject>P-type semiconductors</subject><subject>Semiconductors</subject><subject>Solid State Physics</subject><issn>0361-5235</issn><issn>1543-186X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNp9kE1LAzEQhoMoWKt_wFPA82qS3WSzR_GjCq1KreAtZNOJ3bIma5IKC_54t1bw5mkY5nlfhgehU0rOKSHlRaRUiCIjLM8o4TTP5B4aUV4MqxSv-2hEckEzznJ-iI5iXBNCOZV0hL7mvgXsLZ7pxuFJ8JsOP3j3Dkm3-Np32qWIvcNpBfimBZOCd43BT8F3EFIDcZvdHhfmmeGZd77VPQQ8h0_QLSxx3eNrcLFJPb7dOJMa74bmxQp86I_RgdVthJPfOUYvtzeLq7ts-ji5v7qcZoaVJGWVNVYwyWwtC1rauqaCcSMkMFIzLsBYS3RRk-UyJ6IkpR6QqpK8WFZFAcbkY3S26-2C_9hATGrtN2H4IyomC16JilRyoNiOMsHHGMCqLjTvOvSKErW1rHaW1WBZ_VhW21C-C8UBdm8Q_qr_SX0D0xWA7A</recordid><startdate>20230901</startdate><enddate>20230901</enddate><creator>Widya</creator><creator>Marlina, Lala Adetia</creator><creator>Hutama, Aulia Sukma</creator><creator>Prasetyo, Niko</creator><general>Springer US</general><general>Springer Nature B.V</general><scope>AAYXX</scope><scope>CITATION</scope><scope>3V.</scope><scope>7XB</scope><scope>88I</scope><scope>8AF</scope><scope>8AO</scope><scope>8FE</scope><scope>8FG</scope><scope>8FK</scope><scope>8G5</scope><scope>ABJCF</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>D1I</scope><scope>DWQXO</scope><scope>GNUQQ</scope><scope>GUQSH</scope><scope>HCIFZ</scope><scope>KB.</scope><scope>L6V</scope><scope>M2O</scope><scope>M2P</scope><scope>M7S</scope><scope>MBDVC</scope><scope>P5Z</scope><scope>P62</scope><scope>PDBOC</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PTHSS</scope><scope>Q9U</scope><scope>S0X</scope><orcidid>https://orcid.org/0000-0002-3322-9421</orcidid></search><sort><creationdate>20230901</creationdate><title>Role of Main Group Nonmetal Dopants on the Electronic Properties of the TcS2 Monolayer Revealed by Density Functional Theory</title><author>Widya ; Marlina, Lala Adetia ; Hutama, Aulia Sukma ; Prasetyo, Niko</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c270t-9fcf6282fb8417fbb1625c68e20b256ecff0a4b0dd306707afbb99854d944ecc3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>Characterization and Evaluation of Materials</topic><topic>Chemistry and Materials Science</topic><topic>Density functional theory</topic><topic>Dopants</topic><topic>Electronics and Microelectronics</topic><topic>Energy of formation</topic><topic>First principles</topic><topic>Free energy</topic><topic>Heat of formation</topic><topic>Instrumentation</topic><topic>Magnetic properties</topic><topic>Materials Science</topic><topic>Monolayers</topic><topic>N-type semiconductors</topic><topic>Nanomaterials</topic><topic>Nonmetals</topic><topic>Optical and Electronic Materials</topic><topic>Optoelectronic devices</topic><topic>Original Research Article</topic><topic>P-type semiconductors</topic><topic>Semiconductors</topic><topic>Solid State Physics</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Widya</creatorcontrib><creatorcontrib>Marlina, Lala Adetia</creatorcontrib><creatorcontrib>Hutama, Aulia Sukma</creatorcontrib><creatorcontrib>Prasetyo, Niko</creatorcontrib><collection>CrossRef</collection><collection>ProQuest Central (Corporate)</collection><collection>ProQuest Central (purchase pre-March 2016)</collection><collection>Science Database (Alumni Edition)</collection><collection>STEM Database</collection><collection>ProQuest Pharma Collection</collection><collection>ProQuest SciTech Collection</collection><collection>ProQuest Technology Collection</collection><collection>ProQuest Central (Alumni) (purchase pre-March 2016)</collection><collection>Research Library (Alumni Edition)</collection><collection>Materials Science & Engineering Collection</collection><collection>ProQuest Central (Alumni)</collection><collection>ProQuest Central</collection><collection>Advanced Technologies & Aerospace Collection</collection><collection>ProQuest Central Essentials</collection><collection>ProQuest Central</collection><collection>Technology Collection</collection><collection>ProQuest One Community College</collection><collection>ProQuest Materials Science Collection</collection><collection>ProQuest Central</collection><collection>ProQuest Central Student</collection><collection>Research Library Prep</collection><collection>SciTech Premium Collection</collection><collection>Materials Science Database</collection><collection>ProQuest Engineering Collection</collection><collection>ProQuest_Research Library</collection><collection>Science Database</collection><collection>Engineering Database</collection><collection>Research Library (Corporate)</collection><collection>ProQuest advanced technologies & aerospace journals</collection><collection>ProQuest Advanced Technologies & Aerospace Collection</collection><collection>Materials science collection</collection><collection>ProQuest One Academic Eastern Edition (DO NOT USE)</collection><collection>ProQuest One Academic</collection><collection>ProQuest One Academic UKI Edition</collection><collection>Engineering collection</collection><collection>ProQuest Central Basic</collection><collection>SIRS Editorial</collection><jtitle>Journal of electronic materials</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Widya</au><au>Marlina, Lala Adetia</au><au>Hutama, Aulia Sukma</au><au>Prasetyo, Niko</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Role of Main Group Nonmetal Dopants on the Electronic Properties of the TcS2 Monolayer Revealed by Density Functional Theory</atitle><jtitle>Journal of electronic materials</jtitle><stitle>J. Electron. Mater</stitle><date>2023-09-01</date><risdate>2023</risdate><volume>52</volume><issue>9</issue><spage>5931</spage><epage>5945</epage><pages>5931-5945</pages><issn>0361-5235</issn><eissn>1543-186X</eissn><abstract>The electronic properties of
n
- and
p
-type semiconductors using nonmetals (H, B, C, N, O, Si, P, Se, F, Cl, Br, and I) to substitute sulfur in the TcS
2
monolayer were investigated using first-principles methods based on the density functional theory. The H-, B-, C-, N-, Si-, and P-doped systems were
p
-type, whereas the F-doped systems were
n
-type semiconductors. Numerical results showed that these nonmetals induced magnetic properties through the dopant
p
orbital and neighboring Tc atom
d
orbitals. H-, B-, N-, P-, and F-doped systems exhibited semiconducting magnetic nanomaterial features, whereas Cl-, Br-, and I-doped systems exhibited half-metallic magnetic features. The formation energy of the C-doped system was the lowest followed by the O-doped system, compared to that of the other examined systems. Under Tc-rich growth conditions, the preparation of nonmetal-doped TcS
2
was facile and stable because of its negative impurity formation energy. A more significant change was observed at the band edges of the doped systems compared to the pristine TcS
2
monolayer. These results provided fundamental insights into the doped TcS
2
monolayer for application as photocatalysts and spintronic, optoelectronic, and electronic devices.</abstract><cop>New York</cop><pub>Springer US</pub><doi>10.1007/s11664-023-10513-8</doi><tpages>15</tpages><orcidid>https://orcid.org/0000-0002-3322-9421</orcidid></addata></record> |
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source | Springer Nature |
subjects | Characterization and Evaluation of Materials Chemistry and Materials Science Density functional theory Dopants Electronics and Microelectronics Energy of formation First principles Free energy Heat of formation Instrumentation Magnetic properties Materials Science Monolayers N-type semiconductors Nanomaterials Nonmetals Optical and Electronic Materials Optoelectronic devices Original Research Article P-type semiconductors Semiconductors Solid State Physics |
title | Role of Main Group Nonmetal Dopants on the Electronic Properties of the TcS2 Monolayer Revealed by Density Functional Theory |
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