• Journal of Semiconductors
  • Vol. 42, Issue 12, 122002 (2021)
Xiaoshu Guo1 and Sandong Guo2
Author Affiliations
  • 1Xi'an University of Posts and Telecommunications, Xi'an 710121, China
  • 2School of Electronic Engineering, Xi'an University of Posts and Telecommunications, Xi'an 710121, China
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    DOI: 10.1088/1674-4926/42/12/122002 Cite this Article
    Xiaoshu Guo, Sandong Guo. Janus MSiGeN4 (M = Zr and Hf) monolayers derived from centrosymmetric β-MA2Z4: A first-principles study[J]. Journal of Semiconductors, 2021, 42(12): 122002 Copy Citation Text show less

    Abstract

    A two-dimensional (2D) MA2Z4 family with and phases has been attracting tremendous interest, the MoSi2N4 and WSi2N4 of which have been successfully fabricated ( Science 369, 670 (2020)). Janus monolayers have been achieved in many 2D families, so it is interesting to construct a Janus monolayer from the MA2Z4 family. In this work, Janus MSiGeN4 (M = Zr and Hf) monolayers are predicted from -MA2Z4, which exhibit dynamic, mechanical and thermal stabilities. It is found that they are indirect band-gap semiconductors by using generalized gradient approximation (GGA) plus spin-orbit coupling (SOC). With biaxial strain from 0.90 to 1.10, the energy band gap shows a nonmonotonic behavior due to a change of conduction band minimum (CBM). A semiconductor to metal transition can be induced by both compressive and tensile strains, and the phase transformation point is about 0.96 for compressive strain and 1.10 for tensile strain. The tensile strain can change the positions of CBM and valence band maximum (VBM), and can also induce the weak Rashba-type spin splitting near CBM. For MSiGeN4 (M = Zr and Hf) monolayers, both an in-plane and out-of-plane piezoelectric response can be produced, when a uniaxial strain in the basal plane is applied, which reveals the potential as piezoelectric 2D materials. The high absorption coefficients in the visible light region suggest that MSiGeN4 (M = Zr and Hf) monolayers have potential photocatalytic applications. Our works provide an idea to achieve a Janus structure from the MA2Z4 family, and can hopefully inspire further research exploring Janus MA2Z4 monolayers.
    $C = \left( {\begin{array}{*{20}{c}} {{C_{11}}} & {{C_{12}}} & 0\\ {{C_{12}}} & {{C_{11}}} & 0\\ 0 & 0 & {({C_{11}} - {C_{12}})/2} \end{array}} \right). $(1)

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    $ C_{11}>0,\; \; C_{66}>0. $(2)

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    $ C_{\rm{2D}} = \frac{C_{11}^2-C_{12}^2}{C_{11}}. $(3)

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    $ e = \left( {\begin{array}{*{20}{c}} {{e_{11}}} & { - {e_{11}}} & 0\\ 0 & 0 & { - {e_{11}}}\\ {{e_{31}}} & {{e_{31}}} & 0 \end{array}} \right), $(4)

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    $ d = \left( {\begin{array}{*{20}{c}} {{d_{11}}} & { - {d_{11}}} & 0\\ 0 & 0 & { - 2{d_{11}}}\\ {{d_{31}}} & {{d_{31}}} & 0 \end{array}} \right). $(5)

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    $ d_{11} = \frac{e_{11}}{C_{11}-C_{12}} ,\quad d_{31} = \frac{e_{31}}{C_{11}+C_{12}}. $(6)

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    $ \varepsilon_2(\omega) = \frac{2\pi e^2}{\Omega \epsilon_0}\sum\limits_{k,v,c}\delta(E^c_k-E^v_k-\hbar\omega)|<\psi^c_k|u.r|\psi^v_k>|^2, $(7)

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    $ \alpha(\omega) = \frac{\sqrt{2}\omega}{c}\left\{\left[\varepsilon_1^2(\omega)+\varepsilon_2^2(\omega)\right]^{1/2}-\varepsilon_1(\omega)\right\}^{\frac{1}{2}}. $(8)

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    Xiaoshu Guo, Sandong Guo. Janus MSiGeN4 (M = Zr and Hf) monolayers derived from centrosymmetric β-MA2Z4: A first-principles study[J]. Journal of Semiconductors, 2021, 42(12): 122002
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