First principles investigation of the substitutional doping of Mn in Mg2Ni phase and the electronic structure of Mg3MnNi2 phase

2011 ◽  
Vol 509 ◽  
pp. S328-S333 ◽  
Author(s):  
L.W. Huang ◽  
O. Elkedim ◽  
R. Hamzaoui
2011 ◽  
Vol 213 ◽  
pp. 483-486
Author(s):  
Fang Gui ◽  
Shi Yun Zhou ◽  
Wan Jun Yan ◽  
Chun Hong Zhang ◽  
Xiao Tian Guo ◽  
...  

The electronic structure and optical properties of Fe1-xMnxSi2 have been studied using the first principle plane-wave pseudo-potential based on the density function theory. Substitutional doping is considered with Mn concentrations of x=0.0625, 0.125, 0.1875 and 0.25, respectively. The calculated results show that the volume of β-FeSi2 increase and the band gap increase with increasing of Mn.


2010 ◽  
Vol 663-665 ◽  
pp. 592-595
Author(s):  
Wan Jun Yan ◽  
Shi Yun Zhou ◽  
Fang Gui ◽  
Chun Hong Zhang ◽  
Xiao Tian Guo ◽  
...  

The electronic structure and optical properties of Fe1-xCoxSi2 have been studied using the first principle plane-wave pseudo-potential based on the density function theory. Substitutional doping is considered with Co concentrations of x=0.0625, 0.125, 0.1875 and 0.25, respectively. The calculated results show that the volume of β-FeSi2 increase and the band gap decrease with increasing of Co.


RSC Advances ◽  
2016 ◽  
Vol 6 (49) ◽  
pp. 43794-43801 ◽  
Author(s):  
Chunyan Xu ◽  
Mingfeng Zhu ◽  
Huiling Zheng ◽  
Xiaobo Du ◽  
Wenquan Wang ◽  
...  

A doping C, Si, O and S can induce the magnetic moments of 1.0μBin buckled arsenene, while the substitutional doping of H, F, B, N and P can not produce the magnetism.


2020 ◽  
Vol 98 (3) ◽  
pp. 233-238 ◽  
Author(s):  
Ji Zhang ◽  
Deming Zhang

First-principles density function theory calculations have been performed on the electronic structure and optical properties of mono-doped and co-doped monoclinic NaTaO3 systems. Doping of certain nonmetal ions (N, C, S, and P) and certain co-dopant pairs (C–N, S–N, P–N, and S–P) is investigated. Our calculations show that substitutional doping of C at a Na site, N at an O site, S at a Na site, and P at a Ta site require smaller formation energy based on the optimized structures of doped NaTaO3. In the case of mono-doped NaTaO3, the results indicate that the band gaps were all narrowed resulting in redshift of the absorption edge. However, for C–N, S–N, P–N, and S–P co-doped systems, though the band gap broadened, the appearance of mid-gap and movement of conduction band minimum (CBM) to Fermi energy led to absorption in the visible range. On the basis of the calculated results on nonmetal doped NaTaO3, we theoretically predicted that mono-doped NaTaO3 is more suitable for photocatalysts of water splitting.


2014 ◽  
Vol 52 (12) ◽  
pp. 1025-1029
Author(s):  
Min-Wook Oh ◽  
Tae-Gu Kang ◽  
Byungki Ryu ◽  
Ji Eun Lee ◽  
Sung-Jae Joo ◽  
...  

2012 ◽  
Vol 54 ◽  
pp. 287-292 ◽  
Author(s):  
Xiao-Jun Chen ◽  
Meng-Xue Zeng ◽  
Ren-Nian Wang ◽  
Zhou-Sheng Mo ◽  
Bi-Yu Tang ◽  
...  

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