{"title":"改变单层 SiS2 电子和磁性能的 Pnictogen 原子置换:DFT 研究","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":"{\"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}","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}
引用次数: 0
摘要
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。
Pnictogen Atom Substitution to Modify the Electronic and Magnetic Properties of SiS2 Monolayer: A DFT Study
The density functional theory (DFT) is employed to study the modulation of electronic and magnetic properties of monolayer through doping with pnictogen (P and As) atoms. 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 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 , respectively. Herein, magnetic properties are produced mainly by the outermost 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 monolayer with pnictogen atoms.
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
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method development, numerical methods, statistics