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First-principles study of structure prediction and electronic properties of two-dimensional SiP2 allotropes

Zhou Jia-Jian Zhang Yu-Wen He Chao-Yu Ouyang Tao Li Jin Tang Chao

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First-principles study of structure prediction and electronic properties of two-dimensional SiP2 allotropes

Zhou Jia-Jian, Zhang Yu-Wen, He Chao-Yu, Ouyang Tao, Li Jin, Tang Chao
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  • Since the successful preparation of single-layer graphene in 2004, the two-dimensional (2D) materials have received widespread attention. Driven by this research upsurge, many kinds of 2D compound materials with different properties have been discovered one after another, and some of these 2D materials have a variety of allotropes, showing more abundant properties. Our computational studies focus on searching for new stable 2D SiP2 allotropes, and studying their binding energy, phonon dispersions, electronic band structures, strain-dependent bandgap modulation behaviors, piezoelectric properties, etc. In this paper, three novel 2D SiP2 allotrope structures, i.e. α-SiP2, β-SiP2, and γ-SiP2, are found by the random prediction method of crystal structure based on group theory and graph theory (RG2). Their stabilities and electronic properties are investigated by using the first-principles method based on the density functional theory. The results show that the three novel SiP2 structures are stable thermodynamically, dynamically and mechanically. Using the GW calculations, three novel SiP2 structures possess indirect band gaps of 2.62, 2.99 and 3.00 eV, respectively. Their band gaps are feasible to modulate effectively by applying strain. The band gaps of the three novel SiP2 isomers are reduced significantly when subjected to a large strainused, and the three novel SiP2 isomers exhibit indirect-to-direct bandgap transitions when experienced by a certain strain along the x-axis direction. These properties make them potential materials that are suitable for serving as nanoscale photocatalysts. Moreover, three SiP2 isomers have non-centrosymmetric crystal structures, which enable them to exhibit their piezoelectricities. Therefore, we study their piezoelectric properties by combining the Berry phase theory. Our studies show that three novel 2D SiP2 allotropes have good piezoelectric properties. The piezoelectric coefficient of the α-SiP2 isomer and the β-SiP2 isomer are both larger than that of h-BN, and they are comparable to the counterpart of MoS2. These novel structures promise to be used to fabricate nano-electromechanical devices for micro- and nano-scaled electromechanical conversion and electromechanical sensing and controlling.
      Corresponding author: Tang Chao, tang_chao@xtu.edu.cn
    • Funds: Project supported by the National Natural Science Foundation of China (Grant Nos. 11974299, 11974300) and the Research Foundation of Education Bureau of Hunan Province, China (Grant Nos. 20A503, 20K127).
    [1]

    Novoselov K S, Geim A K, Morozov S V, Jiang D, Zhang Y, Dubonos S V, Grigorieva I V, Firsov A A 2004 Science 306 666Google Scholar

    [2]

    Zhang Y B, Tan Y W, Stormer H L, Kim P 2005 Nature 438 201Google Scholar

    [3]

    Mak K F, Lee C, Hone J, Shan J, Heinz T F 2010 Phys. Rev. Lett. 105 136805Google Scholar

    [4]

    Topsakal M, Aktuerk E, Ciraci S 2009 Phys. Rev. B 79 115442Google Scholar

    [5]

    Cahangirov S, Topsakal M, Akturk E, Sahin H, Ciraci S 2009 Phys. Rev. Lett. 102 236804Google Scholar

    [6]

    Li L, Yu Y, Ye G, Ge Q, Ou X, Wu H, Feng D, Chen, Xian H, Zhang Y B 2014 Nature Nanotechnology 9 372Google Scholar

    [7]

    Liu H, Neal A T, Zhu Z, Luo Z, Xu X F, Tomanek D, Ye P D 2014 ACS Nano 8 4033Google Scholar

    [8]

    Li T, Eugenio C, Daniele C, Carlo G, Marco F, Madan D, Alessandro M, Deji A 2015 Nat. Nanotechnol. 10 227Google Scholar

    [9]

    Duerloo K-A N, Ong M T, Reed E J 2012 J. Phys. Chem. Lett. 3 2871Google Scholar

    [10]

    Fazel S, Jae R H, Hong S K 2017 J. Mater. Chem. A 5 22146Google Scholar

    [11]

    Guo J, Liu Y, Ma Y, Zhu E B, Lee S, Lu Z X, Zhao Z P, Xu C H, Lee S J, Wu H, Kovnir K, Huang Y, Duan X F 2018 Adv. Mater. 30 e1705934Google Scholar

    [12]

    Yang S X, Yang Y H, Wu M H, Hu C G, Shen W F, Gong Y J, Huang L, Jiang C H, Zhang Y Z, Ajayan P M 2018 Adv. Funct. Mater. 28 1707379Google Scholar

    [13]

    Zhou L Q, Guo Y, Zhao J J 2018 Physica E Low Dimens. Syst. Nanostruct. 95 149Google Scholar

    [14]

    Li L, Gong P L, Sheng D P, Wang S A, Wang W K, Zhu X D, Shi X Q, Wang F K, Han W, Yang S J, Liu K L, Li H Q, Zhai T Y 2018 Adv. Mater. 30 e1804541Google Scholar

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    Wadsten T 1967 Acts Chem. Scand. 21 1374

    [16]

    Matta S K, Zhang C, Jiao Y, O, Mullane A, Du A 2018 Nanoscale 10 6369Google Scholar

    [17]

    Xu Y, Li Z, He C, Li J, Ouyang T, Zhang C, Tang C, Zhong J 2020 Appl. Phys. Lett. 116 023103Google Scholar

    [18]

    Xi F, Yang H Y, Ling F, He C Z, Hou J R, Guo J Y, Li L M 2021 Chin. Chem. Lett. 32 1089Google Scholar

    [19]

    Shi X Z, He C Y, Pickard C J, Tang C, Zhong J X 2018 Phys. Rev. B 97 014104Google Scholar

    [20]

    King-Smith R D, Vanderbilt D 1993 Phys. Rev. B 47 1651Google Scholar

    [21]

    Vanderbilt D 2000 J. Phys. Chem. Solids 61 147Google Scholar

    [22]

    Blöchl P E 1994 Phys. Rev. B 50 17953Google Scholar

    [23]

    Kresse G, Joubert D 1999 Phys. Rev. B 59 1758

    [24]

    Kresse G, Furthmüller J 1996 Phys. Rev. B 54 11169Google Scholar

    [25]

    Kresse G, Furthmüller J 1996 Comput. Mater. Sci. 6 15Google Scholar

    [26]

    Perdew J P, Burke K, Ernzerhof M 1996 Phys. Rev. Lett. 77 3865Google Scholar

    [27]

    Grimme S, Antony J, Ehrlich S, Krieg H 2010 J. Chem. Phys. 132 154104Google Scholar

    [28]

    Gomes L C, Carvalho A, Neto A H C 2015 Phys. Rev. B 92 214103Google Scholar

    [29]

    Ni M, Leung M K H, Leung D Y C, Sumathy K 2006 Renew. Sust. Energ. Rev. 11 401

    [30]

    Roldan R, Castellanos-Gomez A, Cappelluti E, Guinea F 2015 J. Phys. Condens. Matter 27 313201Google Scholar

    [31]

    Zhu C R, Wang G, Liu B L, Marie X, Qiao X F, Zhang X, Wu X X, Fan H, Tan P H, Amand T, Urbaszek B 2013 Phys. Rev. B 88 121301Google Scholar

    [32]

    Conley H J, Wang B, Ziegler J I, Haglund R F Jr, Pantelides S T, Bolotin K I 2013 Nano Lett. 13 3626Google Scholar

    [33]

    Fei R, Li W, Li J, Yang L 2015 Appl. Phys. Lett. 107 173104Google Scholar

    [34]

    Blonsky M N, Zhuang H L, Singh A K, Hennig R G 2015 ACS Nano 9 9885Google Scholar

    [35]

    Sevik C, Çakır D, Gülseren O, Peeters F M 2016 J. Phys. Chem. C 120 13948Google Scholar

    [36]

    Michel K H, Verberck B 2009 Phys. Rev. B 80 224301Google Scholar

    [37]

    Liu S, Cohen R 2017 Phys. Rev. Lett. 119 207601Google Scholar

  • 图 1  3种SiP2同素异构体及r-SiP2结构的俯视图(上图)和侧视图(下图) (a) α-SiP2; (b) β-SiP2; (c) γ-SiP2; (d) r-SiP2[14], 红色和绿色分别代表P和Si原子

    Figure 1.  Top view and side view of three SiP2 allotropes and r-SiP2 structure: (a) α-SiP2; (b) β-SiP2; (c) γ-SiP2; (d) r-SiP2[14]. Red and green balls represent P and Si atoms, respectively.

    图 2  3种SiP2异构体声子谱 (a) α-SiP2; (b) β-SiP2; (c) γ-SiP2

    Figure 2.  Phonon dispersion of three SiP2 isomers: (a) α-SiP2; (b) β-SiP2; (c) γ-SiP2.

    图 3  3种SiP2异构体电子能带结构 (a) α-SiP2; (b) β-SiP2; (c) γ-SiP2, 其中红线和黑线分别为GW和HSE的计算结果

    Figure 3.  Electronic band structures of three SiP2 isomers: (a) α-SiP2; (b) β-SiP2; (c) γ-SiP2. The red and black lines are the calculation results of GW and HSE, respectively.

    图 4  3种SiP2异构体的带边位置, 其中虚线为用于水分解的标准氧化还原电势.

    Figure 4.  Band edge positions of three SiP2 isomers, the dashed line is the standard redox potential for water splitting.

    图 5  3种SiP2异构体施加应变后电子带隙的变化, 其中x轴正值表示拉伸应变, 负值表示压缩应变

    Figure 5.  Changes in the electronic band gaps of three SiP2 isomers after applying straining, where positive values along the x-axis represent tensile strain and negative values represent compressive strain.

    图 6  3种SiP2异构体沿x轴方向施加应变后间接-直接带隙转变过程 (a) α-SiP2; (b) β-SiP2; (c) γ-SiP2

    Figure 6.  Indirect-irect band gap transition processes of three SiP2 isomers after applying strain along the x-axis: (a) α-SiP2; (b) β-SiP2; (c) γ-SiP2.

    图 7  3种SiP2异构体施加单轴应变后沿x轴晶胞极化矢量变化

    Figure 7.  Changes in the polarization vector of the unit cell along the x-axis for three SiP2 isomers after applying uniaxial strain.

    表 1  优化后的3种SiP2同素异构体及r-SiP2[16]结构晶格常数、形成能(Eb)和带隙值(Eg)

    Table 1.  Optimized lattice parameters, binding energy (Eb), and band gap values (Eg) of three SiP2 allotropes and r-SiP2[16] structures.

    SystemAb${ {E} }_{\text{b} }\text{/}\text{eV}$${ {E} }_{\text{g} }^{\text{PBE} }\text{/}\text{eV}$${ {E} }_{\text{g} }^{\text{HSE} }\text{/}\text{eV}$${ {E} }_{\text{g} }^{\text{GW} }\text{/}\text{eV}$
    α-SiP26.1313.89–5.381.442.172.62
    β-SiP26.0913.73–5.431.842.612.99
    γ-SiP212.1113.95–5.451.782.553.00
    r-SiP210.003.44–5.471.472.252.63
    DownLoad: CSV

    表 2  3种SiP2异构体的弹性常数Cij (N/m)及压电系数eij (10–10 C/m)和dij (pm/V)

    Table 2.  Calculated elastic coefficients Cij (N/m) and piezoelectric coefficients eij (10–10 C/m) and dij (pm/V) of three SiP2 allotropes.

    System$ {C}_{11} $$ {C}_{22} $$ {C}_{12} $$ {e}_{11} $$ {e}_{12} $$ {d}_{11} $$ {d}_{12} $
    α-SiP269.6965.7414.79–1.050.37–1.710.95
    β-SiP278.3665.4319.10–0.94–0.38–1.13–0.26
    γ-SiP277.6559.9718.04–0.13–0.46–0.01–0.77
    r-SiP2[17]17.94121.778.66–1.930.17–11.220.93
    h-BN[9]291291621.381.380.600.60
    MoS2[9]130130323.643.643.733.73
    DownLoad: CSV
    Baidu
  • [1]

    Novoselov K S, Geim A K, Morozov S V, Jiang D, Zhang Y, Dubonos S V, Grigorieva I V, Firsov A A 2004 Science 306 666Google Scholar

    [2]

    Zhang Y B, Tan Y W, Stormer H L, Kim P 2005 Nature 438 201Google Scholar

    [3]

    Mak K F, Lee C, Hone J, Shan J, Heinz T F 2010 Phys. Rev. Lett. 105 136805Google Scholar

    [4]

    Topsakal M, Aktuerk E, Ciraci S 2009 Phys. Rev. B 79 115442Google Scholar

    [5]

    Cahangirov S, Topsakal M, Akturk E, Sahin H, Ciraci S 2009 Phys. Rev. Lett. 102 236804Google Scholar

    [6]

    Li L, Yu Y, Ye G, Ge Q, Ou X, Wu H, Feng D, Chen, Xian H, Zhang Y B 2014 Nature Nanotechnology 9 372Google Scholar

    [7]

    Liu H, Neal A T, Zhu Z, Luo Z, Xu X F, Tomanek D, Ye P D 2014 ACS Nano 8 4033Google Scholar

    [8]

    Li T, Eugenio C, Daniele C, Carlo G, Marco F, Madan D, Alessandro M, Deji A 2015 Nat. Nanotechnol. 10 227Google Scholar

    [9]

    Duerloo K-A N, Ong M T, Reed E J 2012 J. Phys. Chem. Lett. 3 2871Google Scholar

    [10]

    Fazel S, Jae R H, Hong S K 2017 J. Mater. Chem. A 5 22146Google Scholar

    [11]

    Guo J, Liu Y, Ma Y, Zhu E B, Lee S, Lu Z X, Zhao Z P, Xu C H, Lee S J, Wu H, Kovnir K, Huang Y, Duan X F 2018 Adv. Mater. 30 e1705934Google Scholar

    [12]

    Yang S X, Yang Y H, Wu M H, Hu C G, Shen W F, Gong Y J, Huang L, Jiang C H, Zhang Y Z, Ajayan P M 2018 Adv. Funct. Mater. 28 1707379Google Scholar

    [13]

    Zhou L Q, Guo Y, Zhao J J 2018 Physica E Low Dimens. Syst. Nanostruct. 95 149Google Scholar

    [14]

    Li L, Gong P L, Sheng D P, Wang S A, Wang W K, Zhu X D, Shi X Q, Wang F K, Han W, Yang S J, Liu K L, Li H Q, Zhai T Y 2018 Adv. Mater. 30 e1804541Google Scholar

    [15]

    Wadsten T 1967 Acts Chem. Scand. 21 1374

    [16]

    Matta S K, Zhang C, Jiao Y, O, Mullane A, Du A 2018 Nanoscale 10 6369Google Scholar

    [17]

    Xu Y, Li Z, He C, Li J, Ouyang T, Zhang C, Tang C, Zhong J 2020 Appl. Phys. Lett. 116 023103Google Scholar

    [18]

    Xi F, Yang H Y, Ling F, He C Z, Hou J R, Guo J Y, Li L M 2021 Chin. Chem. Lett. 32 1089Google Scholar

    [19]

    Shi X Z, He C Y, Pickard C J, Tang C, Zhong J X 2018 Phys. Rev. B 97 014104Google Scholar

    [20]

    King-Smith R D, Vanderbilt D 1993 Phys. Rev. B 47 1651Google Scholar

    [21]

    Vanderbilt D 2000 J. Phys. Chem. Solids 61 147Google Scholar

    [22]

    Blöchl P E 1994 Phys. Rev. B 50 17953Google Scholar

    [23]

    Kresse G, Joubert D 1999 Phys. Rev. B 59 1758

    [24]

    Kresse G, Furthmüller J 1996 Phys. Rev. B 54 11169Google Scholar

    [25]

    Kresse G, Furthmüller J 1996 Comput. Mater. Sci. 6 15Google Scholar

    [26]

    Perdew J P, Burke K, Ernzerhof M 1996 Phys. Rev. Lett. 77 3865Google Scholar

    [27]

    Grimme S, Antony J, Ehrlich S, Krieg H 2010 J. Chem. Phys. 132 154104Google Scholar

    [28]

    Gomes L C, Carvalho A, Neto A H C 2015 Phys. Rev. B 92 214103Google Scholar

    [29]

    Ni M, Leung M K H, Leung D Y C, Sumathy K 2006 Renew. Sust. Energ. Rev. 11 401

    [30]

    Roldan R, Castellanos-Gomez A, Cappelluti E, Guinea F 2015 J. Phys. Condens. Matter 27 313201Google Scholar

    [31]

    Zhu C R, Wang G, Liu B L, Marie X, Qiao X F, Zhang X, Wu X X, Fan H, Tan P H, Amand T, Urbaszek B 2013 Phys. Rev. B 88 121301Google Scholar

    [32]

    Conley H J, Wang B, Ziegler J I, Haglund R F Jr, Pantelides S T, Bolotin K I 2013 Nano Lett. 13 3626Google Scholar

    [33]

    Fei R, Li W, Li J, Yang L 2015 Appl. Phys. Lett. 107 173104Google Scholar

    [34]

    Blonsky M N, Zhuang H L, Singh A K, Hennig R G 2015 ACS Nano 9 9885Google Scholar

    [35]

    Sevik C, Çakır D, Gülseren O, Peeters F M 2016 J. Phys. Chem. C 120 13948Google Scholar

    [36]

    Michel K H, Verberck B 2009 Phys. Rev. B 80 224301Google Scholar

    [37]

    Liu S, Cohen R 2017 Phys. Rev. Lett. 119 207601Google Scholar

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  • Received Date:  29 April 2022
  • Accepted Date:  07 July 2022
  • Available Online:  05 December 2022
  • Published Online:  05 December 2022

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