First-Principles Study of Electronic Properties of Substitutionally Doped Monolayer SnP<sub>3</sub>
SnP<sub>3</sub> has a great prospect in electronic and thermoelectric device applications due to its moderate band gap, high carrier mobility, absorption coefficients, and dynamical and chemical stability. Doping in two-dimensional semiconductors is likely to display various anomalous be...
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2022-03-01
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author | Ningxia Zhang Xiaodan Li Shihao Ruan Xiong Chen Shenghao Li Taotao Hu |
author_facet | Ningxia Zhang Xiaodan Li Shihao Ruan Xiong Chen Shenghao Li Taotao Hu |
author_sort | Ningxia Zhang |
collection | DOAJ |
description | SnP<sub>3</sub> has a great prospect in electronic and thermoelectric device applications due to its moderate band gap, high carrier mobility, absorption coefficients, and dynamical and chemical stability. Doping in two-dimensional semiconductors is likely to display various anomalous behaviors when compared to doping in bulk semiconductors due to the significant electron confinement effect. By introducing foreign atoms from group III to VI, we can successfully modify the electronic properties of two-dimensional SnP<sub>3</sub>. The interaction mechanism between the dopants and atoms nearby is also different from the type of doped atom. Both Sn<sub>7</sub>BP<sub>24</sub> and Sn<sub>7</sub>NP<sub>24</sub> systems are indirect bandgap semiconductors, while the Sn<sub>7</sub>AlP<sub>24</sub>, Sn<sub>7</sub>GaP<sub>24</sub>, Sn<sub>7</sub>PP<sub>24,</sub> and Sn<sub>7</sub>AsP<sub>24</sub> systems are metallic due to the contribution of doped atoms intersecting the Fermi level. For all substitutionally doped 2D SnP<sub>3</sub> systems considered here, all metallic systems are nonmagnetic states. In addition, monolayer Sn<sub>7</sub>XP<sub>24</sub> and Sn<sub>8</sub>P<sub>23</sub>Y may have long-range and local magnetic moments, respectively, because of the degree of hybridization between the dopant and its adjacent atoms. The results complement theoretical knowledge and reveal prospective applications of SnP<sub>3</sub>-based electrical nanodevices for the future. |
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issn | 1996-1944 |
language | English |
last_indexed | 2024-03-09T11:41:29Z |
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spelling | doaj.art-6a4a2f5e300644ba8eee257cdb2290642023-11-30T23:32:29ZengMDPI AGMaterials1996-19442022-03-01157246210.3390/ma15072462First-Principles Study of Electronic Properties of Substitutionally Doped Monolayer SnP<sub>3</sub>Ningxia Zhang0Xiaodan Li1Shihao Ruan2Xiong Chen3Shenghao Li4Taotao Hu5College of Science, University of Shanghai for Science and Technology, Shanghai 200093, ChinaCollege of Science, University of Shanghai for Science and Technology, Shanghai 200093, ChinaCollege of Science, University of Shanghai for Science and Technology, Shanghai 200093, ChinaCollege of Science, University of Shanghai for Science and Technology, Shanghai 200093, ChinaCollege of Science, University of Shanghai for Science and Technology, Shanghai 200093, ChinaSchool of Physics, Northeast Normal University, Changchun 130024, ChinaSnP<sub>3</sub> has a great prospect in electronic and thermoelectric device applications due to its moderate band gap, high carrier mobility, absorption coefficients, and dynamical and chemical stability. Doping in two-dimensional semiconductors is likely to display various anomalous behaviors when compared to doping in bulk semiconductors due to the significant electron confinement effect. By introducing foreign atoms from group III to VI, we can successfully modify the electronic properties of two-dimensional SnP<sub>3</sub>. The interaction mechanism between the dopants and atoms nearby is also different from the type of doped atom. Both Sn<sub>7</sub>BP<sub>24</sub> and Sn<sub>7</sub>NP<sub>24</sub> systems are indirect bandgap semiconductors, while the Sn<sub>7</sub>AlP<sub>24</sub>, Sn<sub>7</sub>GaP<sub>24</sub>, Sn<sub>7</sub>PP<sub>24,</sub> and Sn<sub>7</sub>AsP<sub>24</sub> systems are metallic due to the contribution of doped atoms intersecting the Fermi level. For all substitutionally doped 2D SnP<sub>3</sub> systems considered here, all metallic systems are nonmagnetic states. In addition, monolayer Sn<sub>7</sub>XP<sub>24</sub> and Sn<sub>8</sub>P<sub>23</sub>Y may have long-range and local magnetic moments, respectively, because of the degree of hybridization between the dopant and its adjacent atoms. The results complement theoretical knowledge and reveal prospective applications of SnP<sub>3</sub>-based electrical nanodevices for the future.https://www.mdpi.com/1996-1944/15/7/2462first-principlestwo-dimensional materialssubstitutional dopingmonolayer SnP<sub>3</sub> |
spellingShingle | Ningxia Zhang Xiaodan Li Shihao Ruan Xiong Chen Shenghao Li Taotao Hu First-Principles Study of Electronic Properties of Substitutionally Doped Monolayer SnP<sub>3</sub> Materials first-principles two-dimensional materials substitutional doping monolayer SnP<sub>3</sub> |
title | First-Principles Study of Electronic Properties of Substitutionally Doped Monolayer SnP<sub>3</sub> |
title_full | First-Principles Study of Electronic Properties of Substitutionally Doped Monolayer SnP<sub>3</sub> |
title_fullStr | First-Principles Study of Electronic Properties of Substitutionally Doped Monolayer SnP<sub>3</sub> |
title_full_unstemmed | First-Principles Study of Electronic Properties of Substitutionally Doped Monolayer SnP<sub>3</sub> |
title_short | First-Principles Study of Electronic Properties of Substitutionally Doped Monolayer SnP<sub>3</sub> |
title_sort | first principles study of electronic properties of substitutionally doped monolayer snp sub 3 sub |
topic | first-principles two-dimensional materials substitutional doping monolayer SnP<sub>3</sub> |
url | https://www.mdpi.com/1996-1944/15/7/2462 |
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