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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Main Authors: Ningxia Zhang, Xiaodan Li, Shihao Ruan, Xiong Chen, Shenghao Li, Taotao Hu
Format: Article
Language:English
Published: MDPI AG 2022-03-01
Series:Materials
Subjects:
Online Access:https://www.mdpi.com/1996-1944/15/7/2462
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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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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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