Pnictogen Atom Substitution to Modify the Electronic and Magnetic Properties of SiS2 Monolayer: A DFT Study

IF 2.9 4区 工程技术 Q1 MULTIDISCIPLINARY SCIENCES Advanced Theory and Simulations Pub Date : 2024-11-15 DOI:10.1002/adts.202400900
Nguyen Thi Han, J. Guerrero-Sanchez, D. M. Hoat
{"title":"Pnictogen Atom Substitution to Modify the Electronic and Magnetic Properties of SiS2 Monolayer: A DFT Study","authors":"Nguyen Thi Han, J. Guerrero-Sanchez, D. M. Hoat","doi":"10.1002/adts.202400900","DOIUrl":null,"url":null,"abstract":"The density functional theory (DFT) is employed to study the modulation of electronic and magnetic properties of <span data-altimg=\"/cms/asset/58fb9189-d713-4d2d-be99-33ad60c5da8e/adts202400900-math-0003.png\"></span><mjx-container ctxtmenu_counter=\"9\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/adts202400900-math-0003.png\"><mjx-semantics><mjx-msub data-semantic-children=\"0,1\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"upper S i upper S 2\" data-semantic-type=\"subscript\"><mjx-mi data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"2\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\"><mjx-c></mjx-c><mjx-c></mjx-c><mjx-c></mjx-c></mjx-mi><mjx-script style=\"vertical-align: -0.15em;\"><mjx-mn data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"2\" data-semantic-role=\"integer\" data-semantic-type=\"number\" size=\"s\"><mjx-c></mjx-c></mjx-mn></mjx-script></mjx-msub></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:25130390:media:adts202400900:adts202400900-math-0003\" display=\"inline\" location=\"graphic/adts202400900-math-0003.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><msub data-semantic-=\"\" data-semantic-children=\"0,1\" data-semantic-role=\"unknown\" data-semantic-speech=\"upper S i upper S 2\" data-semantic-type=\"subscript\"><mi data-semantic-=\"\" data-semantic-font=\"normal\" data-semantic-parent=\"2\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\">SiS</mi><mn data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic-parent=\"2\" data-semantic-role=\"integer\" data-semantic-type=\"number\">2</mn></msub>${\\rm SiS}_{2}$</annotation></semantics></math></mjx-assistive-mml></mjx-container> monolayer through doping with pnictogen (P and As) atoms. <span data-altimg=\"/cms/asset/2456b317-1617-4eaa-8fb2-e25536afcb33/adts202400900-math-0004.png\"></span><mjx-container ctxtmenu_counter=\"10\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/adts202400900-math-0004.png\"><mjx-semantics><mjx-msub data-semantic-children=\"0,1\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"upper S i upper S 2\" data-semantic-type=\"subscript\"><mjx-mi data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"2\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\"><mjx-c></mjx-c><mjx-c></mjx-c><mjx-c></mjx-c></mjx-mi><mjx-script style=\"vertical-align: -0.15em;\"><mjx-mn data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"2\" data-semantic-role=\"integer\" data-semantic-type=\"number\" size=\"s\"><mjx-c></mjx-c></mjx-mn></mjx-script></mjx-msub></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:25130390:media:adts202400900:adts202400900-math-0004\" display=\"inline\" location=\"graphic/adts202400900-math-0004.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><msub data-semantic-=\"\" data-semantic-children=\"0,1\" data-semantic-role=\"unknown\" data-semantic-speech=\"upper S i upper S 2\" data-semantic-type=\"subscript\"><mi data-semantic-=\"\" data-semantic-font=\"normal\" data-semantic-parent=\"2\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\">SiS</mi><mn data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic-parent=\"2\" data-semantic-role=\"integer\" data-semantic-type=\"number\">2</mn></msub>${\\rm SiS}_{2}$</annotation></semantics></math></mjx-assistive-mml></mjx-container> monolayer is intrinsically non-magnetic, exhibiting the semiconductor nature with indirect bandgap of 1.39(2.26) eV provided by standard(hybrid) functional. This 2D material is metallized under effects of single Si vacancy, single S vacancy, and pair Si─S vacancies. In the latter case, significant magnetism with a total magnetic moment of 1.55 <span data-altimg=\"/cms/asset/3232688e-1302-4c09-abb6-f5c93e72f211/adts202400900-math-0005.png\"></span><mjx-container ctxtmenu_counter=\"11\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/adts202400900-math-0005.png\"><mjx-semantics><mjx-msub data-semantic-children=\"0,1\" data-semantic- data-semantic-role=\"greekletter\" data-semantic-speech=\"mu Subscript upper B\" data-semantic-type=\"subscript\"><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic- data-semantic-parent=\"2\" data-semantic-role=\"greekletter\" data-semantic-type=\"identifier\"><mjx-c></mjx-c></mjx-mi><mjx-script style=\"vertical-align: -0.15em;\"><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic- data-semantic-parent=\"2\" data-semantic-role=\"latinletter\" data-semantic-type=\"identifier\" size=\"s\"><mjx-c></mjx-c></mjx-mi></mjx-script></mjx-msub></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:25130390:media:adts202400900:adts202400900-math-0005\" display=\"inline\" location=\"graphic/adts202400900-math-0005.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><msub data-semantic-=\"\" data-semantic-children=\"0,1\" data-semantic-role=\"greekletter\" data-semantic-speech=\"mu Subscript upper B\" data-semantic-type=\"subscript\"><mi data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic-parent=\"2\" data-semantic-role=\"greekletter\" data-semantic-type=\"identifier\">μ</mi><mi data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic-parent=\"2\" data-semantic-role=\"latinletter\" data-semantic-type=\"identifier\">B</mi></msub>$\\mu _{B}$</annotation></semantics></math></mjx-assistive-mml></mjx-container> is produced mainly by S atoms around the vacancy sites. The monolayer metallization takes place also when doping with P and As atoms at Si sublattice, preserving the nonmagnetic nature. Meanwhile, P and As substitution leads to the emergence of magnetism with total magnetic moments of 0.93 and 0.99 <span data-altimg=\"/cms/asset/c3dd4641-1242-4e29-8934-ce290e6732ef/adts202400900-math-0006.png\"></span><mjx-container ctxtmenu_counter=\"12\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/adts202400900-math-0006.png\"><mjx-semantics><mjx-msub data-semantic-children=\"0,1\" data-semantic- data-semantic-role=\"greekletter\" data-semantic-speech=\"mu Subscript upper B\" data-semantic-type=\"subscript\"><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic- data-semantic-parent=\"2\" data-semantic-role=\"greekletter\" data-semantic-type=\"identifier\"><mjx-c></mjx-c></mjx-mi><mjx-script style=\"vertical-align: -0.15em;\"><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic- data-semantic-parent=\"2\" data-semantic-role=\"latinletter\" data-semantic-type=\"identifier\" size=\"s\"><mjx-c></mjx-c></mjx-mi></mjx-script></mjx-msub></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:25130390:media:adts202400900:adts202400900-math-0006\" display=\"inline\" location=\"graphic/adts202400900-math-0006.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><msub data-semantic-=\"\" data-semantic-children=\"0,1\" data-semantic-role=\"greekletter\" data-semantic-speech=\"mu Subscript upper B\" data-semantic-type=\"subscript\"><mi data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic-parent=\"2\" data-semantic-role=\"greekletter\" data-semantic-type=\"identifier\">μ</mi><mi data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic-parent=\"2\" data-semantic-role=\"latinletter\" data-semantic-type=\"identifier\">B</mi></msub>$\\mu _{B}$</annotation></semantics></math></mjx-assistive-mml></mjx-container>, respectively. Herein, magnetic properties are produced mainly by the outermost <span data-altimg=\"/cms/asset/41f3fb3a-0036-4cda-b38c-2c7d156d7ff8/adts202400900-math-0007.png\"></span><mjx-container ctxtmenu_counter=\"13\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/adts202400900-math-0007.png\"><mjx-semantics><mjx-mi data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic- data-semantic-role=\"latinletter\" data-semantic-speech=\"p\" data-semantic-type=\"identifier\"><mjx-c></mjx-c></mjx-mi></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:25130390:media:adts202400900:adts202400900-math-0007\" display=\"inline\" location=\"graphic/adts202400900-math-0007.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><mi data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"italic\" data-semantic-role=\"latinletter\" data-semantic-speech=\"p\" data-semantic-type=\"identifier\">p</mi>$p$</annotation></semantics></math></mjx-assistive-mml></mjx-container> orbital of pnictogen impurities. Interestingly, the results assert the emergence of the half-metallicity, which gives evidence of new highly spin-polarized 2D materials. Further, doping with pair P/P, As/As, and P/As atoms are also considered with different doping configurations. It is found that the nonmagnetic semiconductor nature is preserved upon doping with pair pnictogen atoms, however, the indirect-to-direct gap transition is induced. Moreover, the energy gap exhibits large reduction between 51.80% and 77.70%. The findings in this work may suggest the formation of prospective optoelectronic and spintronic 2D materials by doping <span data-altimg=\"/cms/asset/ca24c74e-84ca-415f-8bf6-21478f0841b3/adts202400900-math-0008.png\"></span><mjx-container ctxtmenu_counter=\"14\" ctxtmenu_oldtabindex=\"1\" jax=\"CHTML\" role=\"application\" sre-explorer- style=\"font-size: 103%; position: relative;\" tabindex=\"0\"><mjx-math aria-hidden=\"true\" location=\"graphic/adts202400900-math-0008.png\"><mjx-semantics><mjx-msub data-semantic-children=\"0,1\" data-semantic- data-semantic-role=\"unknown\" data-semantic-speech=\"upper S i upper S 2\" data-semantic-type=\"subscript\"><mjx-mi data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"2\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\"><mjx-c></mjx-c><mjx-c></mjx-c><mjx-c></mjx-c></mjx-mi><mjx-script style=\"vertical-align: -0.15em;\"><mjx-mn data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic- data-semantic-parent=\"2\" data-semantic-role=\"integer\" data-semantic-type=\"number\" size=\"s\"><mjx-c></mjx-c></mjx-mn></mjx-script></mjx-msub></mjx-semantics></mjx-math><mjx-assistive-mml display=\"inline\" unselectable=\"on\"><math altimg=\"urn:x-wiley:25130390:media:adts202400900:adts202400900-math-0008\" display=\"inline\" location=\"graphic/adts202400900-math-0008.png\" xmlns=\"http://www.w3.org/1998/Math/MathML\"><semantics><msub data-semantic-=\"\" data-semantic-children=\"0,1\" data-semantic-role=\"unknown\" data-semantic-speech=\"upper S i upper S 2\" data-semantic-type=\"subscript\"><mi data-semantic-=\"\" data-semantic-font=\"normal\" data-semantic-parent=\"2\" data-semantic-role=\"unknown\" data-semantic-type=\"identifier\">SiS</mi><mn data-semantic-=\"\" data-semantic-annotation=\"clearspeak:simple\" data-semantic-font=\"normal\" data-semantic-parent=\"2\" data-semantic-role=\"integer\" data-semantic-type=\"number\">2</mn></msub>${\\rm SiS}_{2}$</annotation></semantics></math></mjx-assistive-mml></mjx-container> monolayer with pnictogen atoms.","PeriodicalId":7219,"journal":{"name":"Advanced Theory and Simulations","volume":"5 1","pages":""},"PeriodicalIF":2.9000,"publicationDate":"2024-11-15","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"Advanced Theory and Simulations","FirstCategoryId":"5","ListUrlMain":"https://doi.org/10.1002/adts.202400900","RegionNum":4,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q1","JCRName":"MULTIDISCIPLINARY SCIENCES","Score":null,"Total":0}
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Abstract

The density functional theory (DFT) is employed to study the modulation of electronic and magnetic properties of SiS2${\rm SiS}_{2}$ monolayer through doping with pnictogen (P and As) atoms. SiS2${\rm SiS}_{2}$ monolayer is intrinsically non-magnetic, exhibiting the semiconductor nature with indirect bandgap of 1.39(2.26) eV provided by standard(hybrid) functional. This 2D material is metallized under effects of single Si vacancy, single S vacancy, and pair Si─S vacancies. In the latter case, significant magnetism with a total magnetic moment of 1.55 μB$\mu _{B}$ is produced mainly by S atoms around the vacancy sites. The monolayer metallization takes place also when doping with P and As atoms at Si sublattice, preserving the nonmagnetic nature. Meanwhile, P and As substitution leads to the emergence of magnetism with total magnetic moments of 0.93 and 0.99 μB$\mu _{B}$, respectively. Herein, magnetic properties are produced mainly by the outermost p$p$ orbital of pnictogen impurities. Interestingly, the results assert the emergence of the half-metallicity, which gives evidence of new highly spin-polarized 2D materials. Further, doping with pair P/P, As/As, and P/As atoms are also considered with different doping configurations. It is found that the nonmagnetic semiconductor nature is preserved upon doping with pair pnictogen atoms, however, the indirect-to-direct gap transition is induced. Moreover, the energy gap exhibits large reduction between 51.80% and 77.70%. The findings in this work may suggest the formation of prospective optoelectronic and spintronic 2D materials by doping SiS2${\rm SiS}_{2}$ monolayer with pnictogen atoms.

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改变单层 SiS2 电子和磁性能的 Pnictogen 原子置换:DFT 研究
本文采用密度泛函理论(DFT)研究了通过掺杂对锑原子(P 原子和 As 原子)来调节单层 SiS2${rm SiS}_{2}$ 的电子和磁性能。SiS2${/rm SiS}_{2}$单层本质上是无磁性的,具有标准(混合)官能团提供的1.39(2.26) eV间接带隙的半导体性质。这种二维材料在单 Si 空位、单 S 空位和成对 Si─S 空位的作用下被金属化。在后一种情况下,主要由空位周围的 S 原子产生明显的磁性,总磁矩为 1.55 μB$\mu _{B}$。在硅亚晶格上掺入 P 原子和 As 原子时,单层金属化也会发生,并保持非磁性。同时,P 原子和 As 原子的取代导致了磁性的出现,总磁矩分别为 0.93 和 0.99 μB$\mu _{B}$。在这里,磁性主要是由 pnictogen 杂质的最外层 p$p$ 轨道产生的。有趣的是,研究结果证实了半金属性的出现,这为新型高自旋极化二维材料提供了证据。此外,还考虑了以不同的掺杂配置掺入成对的 P/P、As/As 和 P/As 原子。研究发现,掺入成对的P/P、As/As和P/As原子后,非磁性半导体性质得以保留,但却诱发了间接到直接间隙的转变。此外,能隙在 51.80% 到 77.70% 之间出现了大幅缩小。这项工作的发现可能表明,通过在 SiS2${\rm SiS}_{2}$ 单层中掺杂对锑原子,有望形成光电和自旋电子二维材料。
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Advanced Theory and Simulations
Advanced Theory and Simulations Multidisciplinary-Multidisciplinary
CiteScore
5.50
自引率
3.00%
发文量
221
期刊介绍: Advanced Theory and Simulations is an interdisciplinary, international, English-language journal that publishes high-quality scientific results focusing on the development and application of theoretical methods, modeling and simulation approaches in all natural science and medicine areas, including: materials, chemistry, condensed matter physics engineering, energy life science, biology, medicine atmospheric/environmental science, climate science planetary science, astronomy, cosmology method development, numerical methods, statistics
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