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基于第一性原理计算, 确定了3种稳定未被报道的Nb2SiTe4基化合物(A2BX4: Nb2SiSe4, Nb2SnTe4和Ta2GeTe4), 研究了其电子结构, 光学性质以及应力工程对其电子结构的调控. 计算结果表明上述3种化合物具有类似Nb2SiTe4的窄带隙值、强的光吸收性能以及显著的光学各向异性, 可用于光电器件之中. 其晶格常数范围为6.04 Å ≤ a ≤ 6.81 Å, 7.74 Å ≤ b ≤ 8.15 Å. Ta2GeTe4的晶格参数与Nb2SiTe4几乎相同, 带隙值减小了0.15 eV, 可应用于远红外光探测. 应力工程表明外加双轴拉伸应力可减小A2BX4体系带隙值. 外加双轴压缩应力时, A2BX4体系价带顶轨道可出现反转(Nb2SiTe4, Nb2GeTe4和Ta2GeTe4), 由B位阳离子占据态d轨道主导转变为B位阳离子占据态d轨道与X位阴离子满p轨道共同主导, 导致带隙值变化趋势异常. 我们预测该价带顶轨道的反转可有效降低空穴有效质量, 促进载流子的迁移, 有助于器件性能的提升.Two-dimensional (2D) niobium silicon telluride (Nb2SiTe4) was recently proposed as a promising candidate in infrared detector, photoelectric conversion, polarized optical sensor and ferroelastic switching application due to its narrow bandgap, long-term air stability, high carrier mobility, etc. However, the in-plane strains and interfacial defects induced by the lattice misfits between functional layers are harmful to 2D heterojunction nanodevice performance, making the crystal-lattice regulation and strain engineering necessary to achieve lattice matching and strain-controllable interface. Here, using first-principles calculations and elemental substitutions, i.e., replacing cations (anions) with elements in the same group of periodic table, we identify three new and stable single-layer A2BX4 analogues (Nb2SiSe4, Nb2SnTe4 and Ta2GeTe4) as appealing candidates in manipulating the lattice parameters of Nb2SiTe4. The controllable lattice parameters are 6.04 Å ≤ a ≤ 6.81 Å and 7.74 Å ≤ b ≤ 8.15 Å. Among them, Ta2GeTe4 exhibits similar lattice parameters to Nb2SiTe4 but smaller bandgap, yielding better response in far-infrared region. Strain engineering shows that the external biaxial tensile stress narrows the bandgaps of A2BX4 due to the downshifting in energy of conduction band minimum (CBM). External biaxial compressive stress induces valance band maximum (VBM) orbital inversion for Nb2SiTe4, Nb2GeTe4 and Ta2GeTe4, which pushes up VBM and discontinues the trend of corresponding bandgap increase. In this case, the bandgap change depends on the competition between energy upshifts of both CBM and VBM. In the Nb2SiSe4 and Nb2SnTe4 cases, the d-p antibonding coupling in valance band is so strong that no valance band inversion appears while the bandgap increases by ~0.3 eV under −5% compressive strain. Regarding Nb2SiTe4, Nb2GeTe4 and Ta2GeTe4, their bandgaps can hardly change under −5% compressive strain, indicating that the energy upshift in VBM equals that in CBM. Such a valance band inversion is attributed to Te outmost p orbital overlapping, which introduces more dispersive VBM and smaller effective mass of hole. Our findings suggest that Nb2SiTe4 can be alloyed with Nb2SiSe4, Nb2SnTe4 and Ta2GeTe4 to achieve controllable device lattice matching while maintaining its superior properties at the same time. The use of external biaxial compressive stress can promote the hole diffusion and improve the device performance.
[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] Fan Y, Liu X, Wang J, Ai H, Zhao M 2018 Phys. Chem. Chem. Phys. 20 11369Google Scholar
[3] Son Y W, Cohen M L, Louie S G 2006 Phys. Rev. Lett. 97 216803Google Scholar
[4] Qiao Z, Ren W, Chen H, Bellaiche L, Zhang Z, Macdonald A H, Niu Q 2014 Phys. Rev. Lett. 112 116404Google Scholar
[5] Ishii T, Sato T 1983 J. Cryst. Growth 61 689Google Scholar
[6] Radisavljevic B, Radenovic A, Brivio J, Giacometti V, Kis A 2011 Nat. Nanotechnol. 6 147Google Scholar
[7] Qiao J, Kong X, Hu Z X, Yang F, Ji W 2014 Nat. Commun. 5 4475Google Scholar
[8] Venkatasubramanian R, Colpitts T, Watko E, Lamvik M, El-Masry N 1997 J. Cryst. Growth 170 817Google Scholar
[9] Zhao M, Xia W, Wang Y, Luo M, Tian Z, Guo Y, Hu W, Xue J 2019 ACS Nano 13 10705Google Scholar
[10] Fang W Y, Li P A, Yuan J H, Xue K H, Wang J F 2019 J. Electron. Mater. 49 959Google Scholar
[11] Zhang T, Ma Y, Xu X, Lei C, Huang B, Dai Y 2020 J. Phys. Chem. Lett. 11 497Google Scholar
[12] Jain S C, Harker A H, Cowley R A 1997 Philos. Mag. A 75 1461Google Scholar
[13] Wosinski T, Yastrubchak O, Makosa A, Figielski T 2000 J. Phys. Condens. Matter 12 10153Google Scholar
[14] Smith A M, Mohs A M, Nie S 2009 Nat. Nanotechnol. 4 56Google Scholar
[15] Perdew J P, Burke K, Ernzerhof M 1996 Phys. Rev. Lett. 77 3865Google Scholar
[16] Kresse G, Joubert D 1999 Phys. Rev. B 59 1758Google Scholar
[17] Monkhorst H J, Pack J D 1976 Phys. Rev. B 13 5188Google Scholar
[18] Heyd J, Scuseria G E, Ernzerhof M 2003 J. Chem. Phys. 118 8207Google Scholar
[19] Togo A, Tanaka I 2015 Scr. Mater. 108 1Google Scholar
[20] Jain A, Ong S P, Hautier G, Chen W, Richards W D, Dacek S, Cholia S, Gunter D, Skinner D, Ceder G, Persson K A 2013 APL Mater. 1 011002Google Scholar
[21] Tremel W, Kleinke H, Derstroff V, Reisner C 1995 J. Alloys. Compd. 219 73Google Scholar
[22] Gareh J, Boucher F, Evain M 1996 Eur. J. Solid State Inorg. Chem. 33 355
[23] Snyder G J, Caillat T, Fleurial J P 2011 J. Mater. Res. 15 2789Google Scholar
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图 1 (a) 二维A2BX4化合物的晶体结构图; (b)—(f) 筛选出的5种稳定A2BX4化合物的化学势能窗口图, 分别对应Nb2SiTe4, Nb2GeTe4, Nb2SiSe4, Nb2SnTe4和Ta2GeTe4.
Fig. 1. (a) Crystal structure of A2BX4 compounds; (b)–(f) Chemical potential windows for 5 stable A2BX4 compounds corresponding to Nb2SiTe4, Nb2GeTe4, Nb2SiSe4, Nb2SnTe4 and Ta2GeTe4, respectively.
图 3 HSE06计算的能带结构 (a) Nb2SiSe4; (b) Nb2SiTe4; (c) Nb2GeTe4; (d) Nb2SnTe4; (e) Ta2GeTe4. 其中蓝线(绿线)代表Nb2SiTe4的VBM(CBM)位置, 数字表示相比Nb2SiTe4 VBM(CBM)的移动
Fig. 3. HSE06 calculated band structures for (a) Nb2SiSe4, (b) Nb2SiTe4, (c) Nb2GeTe4, (d) Nb2SnTe4 and (e) Ta2GeTe4, respectively. Lines represent for VBM (blue) and CBM (green) of Nb2SiTe4. Numbers indicate VBM(CBM) shifts compared with Nb2SiTe4.
图 5 PBE计算的外加 ± 5%应力时A2BX4的能带结构图 (a) Nb2SiSe4; (b) Nb2SiTe4; (c) Nb2GeTe4; (d) Nb2SnTe4; (e) Ta2GeTe4; (f), (g), (h)为对应外应力下Nb2SiTe4 VBM的电荷密度图
Fig. 5. PBE calculated band structures for A2BX4 under ± 5% strain: (a) Nb2SiSe4; (b) Nb2SiTe4; (c) Nb2GeTe4; (d) Nb2SnTe4; (e) Ta2GeTe4; (f), (g), (h) VBM charge density maps of Nb2SiTe4 under strains.
表 1 A2BX4化合物的理论晶格常数与带隙值
Table 1. Theoretical lattice constants and bandgaps of stable A2BX4 compounds.
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[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] Fan Y, Liu X, Wang J, Ai H, Zhao M 2018 Phys. Chem. Chem. Phys. 20 11369Google Scholar
[3] Son Y W, Cohen M L, Louie S G 2006 Phys. Rev. Lett. 97 216803Google Scholar
[4] Qiao Z, Ren W, Chen H, Bellaiche L, Zhang Z, Macdonald A H, Niu Q 2014 Phys. Rev. Lett. 112 116404Google Scholar
[5] Ishii T, Sato T 1983 J. Cryst. Growth 61 689Google Scholar
[6] Radisavljevic B, Radenovic A, Brivio J, Giacometti V, Kis A 2011 Nat. Nanotechnol. 6 147Google Scholar
[7] Qiao J, Kong X, Hu Z X, Yang F, Ji W 2014 Nat. Commun. 5 4475Google Scholar
[8] Venkatasubramanian R, Colpitts T, Watko E, Lamvik M, El-Masry N 1997 J. Cryst. Growth 170 817Google Scholar
[9] Zhao M, Xia W, Wang Y, Luo M, Tian Z, Guo Y, Hu W, Xue J 2019 ACS Nano 13 10705Google Scholar
[10] Fang W Y, Li P A, Yuan J H, Xue K H, Wang J F 2019 J. Electron. Mater. 49 959Google Scholar
[11] Zhang T, Ma Y, Xu X, Lei C, Huang B, Dai Y 2020 J. Phys. Chem. Lett. 11 497Google Scholar
[12] Jain S C, Harker A H, Cowley R A 1997 Philos. Mag. A 75 1461Google Scholar
[13] Wosinski T, Yastrubchak O, Makosa A, Figielski T 2000 J. Phys. Condens. Matter 12 10153Google Scholar
[14] Smith A M, Mohs A M, Nie S 2009 Nat. Nanotechnol. 4 56Google Scholar
[15] Perdew J P, Burke K, Ernzerhof M 1996 Phys. Rev. Lett. 77 3865Google Scholar
[16] Kresse G, Joubert D 1999 Phys. Rev. B 59 1758Google Scholar
[17] Monkhorst H J, Pack J D 1976 Phys. Rev. B 13 5188Google Scholar
[18] Heyd J, Scuseria G E, Ernzerhof M 2003 J. Chem. Phys. 118 8207Google Scholar
[19] Togo A, Tanaka I 2015 Scr. Mater. 108 1Google Scholar
[20] Jain A, Ong S P, Hautier G, Chen W, Richards W D, Dacek S, Cholia S, Gunter D, Skinner D, Ceder G, Persson K A 2013 APL Mater. 1 011002Google Scholar
[21] Tremel W, Kleinke H, Derstroff V, Reisner C 1995 J. Alloys. Compd. 219 73Google Scholar
[22] Gareh J, Boucher F, Evain M 1996 Eur. J. Solid State Inorg. Chem. 33 355
[23] Snyder G J, Caillat T, Fleurial J P 2011 J. Mater. Res. 15 2789Google Scholar
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