Tunable band gap Cu2ZnSnS4xSe4(1−x) nanocrystals: experimental and first-principles calculations

CrystEngComm ◽  
2011 ◽  
Vol 13 (7) ◽  
pp. 2222 ◽  
Author(s):  
Hao Wei ◽  
Zichao Ye ◽  
Meng Li ◽  
Yanjie Su ◽  
Zhi Yang ◽  
...  
RSC Advances ◽  
2015 ◽  
Vol 5 (94) ◽  
pp. 77154-77158 ◽  
Author(s):  
Zhen-Kun Tang ◽  
Wei-Wei Liu ◽  
Deng-Yu Zhang ◽  
Woon-Ming Lau ◽  
Li-Min Liu

The electronic structures and magnetic properties of two dimensional (2D) hexagonal Ni(OH)2 are explored based on first-principles calculations.


2020 ◽  
Vol 22 (39) ◽  
pp. 22520-22528
Author(s):  
Tong Chen ◽  
Huili Li ◽  
Yuyuan Zhu ◽  
Desheng Liu ◽  
Guanghui Zhou ◽  
...  

We investigate the tunable band-gap semiconductor characteristics and electronic transport behaviors of 2D and quasi-1D CP derivatives by using first-principle methods. With bi-axial strain, the band gaps display an incremental trend from compression to stretching.


2011 ◽  
Vol 21 (34) ◽  
pp. 12605 ◽  
Author(s):  
Hao Wei ◽  
Yanjie Su ◽  
Shangzhi Chen ◽  
Yang Lin ◽  
Zhi Yang ◽  
...  

Nanoscale ◽  
2018 ◽  
Vol 10 (24) ◽  
pp. 11553-11563 ◽  
Author(s):  
Huimin Sun ◽  
Junyong Wang ◽  
Fang Wang ◽  
Liping Xu ◽  
Kai Jiang ◽  
...  

We report enhanced exciton emission behavior of W(SxSe1−x)2 monolayers with changing the sulfur content derived by the CVD method.


RSC Advances ◽  
2015 ◽  
Vol 5 (102) ◽  
pp. 83876-83879 ◽  
Author(s):  
Chengyong Xu ◽  
Paul A. Brown ◽  
Kevin L. Shuford

We have investigated the effect of uniform plane strain on the electronic properties of monolayer 1T-TiS2using first-principles calculations. With the appropriate tensile strain, the material properties can be transformed from a semimetal to a direct band gap semiconductor.


Nanomaterials ◽  
2018 ◽  
Vol 8 (11) ◽  
pp. 876 ◽  
Author(s):  
Qi Qian ◽  
Lei Peng ◽  
Yu Cui ◽  
Liping Sun ◽  
Jinyan Du ◽  
...  

We systematically study, by using first-principles calculations, stabilities, electronic properties, and optical properties of GexSn1-xSe alloy made of SnSe and GeSe monolayers with different Ge concentrations x = 0.0, 0.25, 0.5, 0.75, and 1.0. Our results show that the critical solubility temperature of the alloy is around 580 K. With the increase of Ge concentration, band gap of the alloy increases nonlinearly and ranges from 0.92 to 1.13 eV at the PBE level and 1.39 to 1.59 eV at the HSE06 level. When the Ge concentration x is more than 0.5, the alloy changes into a direct bandgap semiconductor; the band gap ranges from 1.06 to 1.13 eV at the PBE level and 1.50 to 1.59 eV at the HSE06 level, which falls within the range of the optimum band gap for solar cells. Further optical calculations verify that, through alloying, the optical properties can be improved by subtle controlling the compositions. Since GexSn1-xSe alloys with different compositions have been successfully fabricated in experiments, we hope these insights will contribute to the future application in optoelectronics.


2005 ◽  
Vol 475-479 ◽  
pp. 3095-3098
Author(s):  
Katsuyuki Matsunaga ◽  
Teruyasu Mizoguchi ◽  
Atsutomo Nakamura ◽  
Takahisa Yamamoto ◽  
Yuichi Ikuhara

First-principles pseudopotential calculations were performed to investigate atomic and electronic structures of titanium (Ti) dopants in alumina (Al2O3). It was found that a substitutional Ti3+ defect induced an extra level occupied by one electron within the band gap of Al2O3. When two or more substitutional Ti3+ defects were located closely to each other, the defect-induced levels exhibited strong bonding interactions, and their formation energies decreased with increasing numbers of Ti3+ defects. This indicates that association and clustering of substitutional Ti3+ defects in Al2O3 can take place due to the interaction of the defect-induced levels.


RSC Advances ◽  
2016 ◽  
Vol 6 (34) ◽  
pp. 28484-28488 ◽  
Author(s):  
Dandan Wang ◽  
DongXue Han ◽  
Lei Liu ◽  
Li Niu

Graphene band gap opening is achieved when integrated with C2N. C2N/graphene heterostructures are promising materials for FETs and water splitting.


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