TY - JOUR
T1 - Electronic and mechanical properties of ScX i (X= S, Se) monolayers and their heterostructures
AU - Rao, Lixiang
AU - Tang, Gang
AU - Hong, Jiawang
N1 - Publisher Copyright:
© 2023 American Physical Society.
PY - 2023/1
Y1 - 2023/1
N2 - Inspired by the successful synthesis of bulk ScSI in a recent work [Ferrenti et al., Chem. Mater. 34, 5443 (2022)10.1021/acs.chemmater.2c00318], we have systematically investigated the mechanical and electronic properties of ScXI (X=S,Se) monolayers and their heterostructures by using first-principles calculations. Our calculations verify the experimental speculation that the bulk ScSI is readily exfoliatable and the monolayers of ScXI (X=S,Se) are stable. The Young's moduli with strong anisotropy (50.2-91.5Nm-1) of ScXI monolayers are comparable to those of phosphorene (26-105Nm-1), but smaller than those of isotropic graphene (349Nm-1), MoS2 (122.3Nm-1), and h-BN (276Nm-1), indicating their lower stiffness. In addition, ScSI/ScSeI monolayers show good flexibility with critical strain of 29%/33%. Application of strain can effectively regulate the band gap (Eg) and band edge of ScXI (X=S,Se) monolayers. For instance, the Eg of the ScSeI monolayer is reduced from 1.83 to 1.59 eV and the band gap type is changed from indirect to direct band gap when a compressive strain of 6% is applied along the x direction, which is attributed to the orbital hybridization between the d orbital of Sc and p orbital of the elements at the X and I sites. More importantly, ScXI (X=S,Se) monolayers can form type II vertical heterostructure with typical two-dimensional semiconductors due to the deeper energy levels of their valence band maximum and conduction band minimum. In addition, ScXI (X=S,Se) monolayers can also be used to form type I lateral heterostructure with the ScSeBr monolayer. The excellent ductility, strain-tuned electronic properties, and heterostructure design make ScXI (X=S,Se) monolayers promising candidates for the application of flexible electronic devices.
AB - Inspired by the successful synthesis of bulk ScSI in a recent work [Ferrenti et al., Chem. Mater. 34, 5443 (2022)10.1021/acs.chemmater.2c00318], we have systematically investigated the mechanical and electronic properties of ScXI (X=S,Se) monolayers and their heterostructures by using first-principles calculations. Our calculations verify the experimental speculation that the bulk ScSI is readily exfoliatable and the monolayers of ScXI (X=S,Se) are stable. The Young's moduli with strong anisotropy (50.2-91.5Nm-1) of ScXI monolayers are comparable to those of phosphorene (26-105Nm-1), but smaller than those of isotropic graphene (349Nm-1), MoS2 (122.3Nm-1), and h-BN (276Nm-1), indicating their lower stiffness. In addition, ScSI/ScSeI monolayers show good flexibility with critical strain of 29%/33%. Application of strain can effectively regulate the band gap (Eg) and band edge of ScXI (X=S,Se) monolayers. For instance, the Eg of the ScSeI monolayer is reduced from 1.83 to 1.59 eV and the band gap type is changed from indirect to direct band gap when a compressive strain of 6% is applied along the x direction, which is attributed to the orbital hybridization between the d orbital of Sc and p orbital of the elements at the X and I sites. More importantly, ScXI (X=S,Se) monolayers can form type II vertical heterostructure with typical two-dimensional semiconductors due to the deeper energy levels of their valence band maximum and conduction band minimum. In addition, ScXI (X=S,Se) monolayers can also be used to form type I lateral heterostructure with the ScSeBr monolayer. The excellent ductility, strain-tuned electronic properties, and heterostructure design make ScXI (X=S,Se) monolayers promising candidates for the application of flexible electronic devices.
UR - http://www.scopus.com/inward/record.url?scp=85147512224&partnerID=8YFLogxK
U2 - 10.1103/PhysRevMaterials.7.014010
DO - 10.1103/PhysRevMaterials.7.014010
M3 - Article
AN - SCOPUS:85147512224
SN - 2475-9953
VL - 7
JO - Physical Review Materials
JF - Physical Review Materials
IS - 1
M1 - 014010
ER -