Pressure effect on the mechanical and electronic properties of B3N3: A first-principle study

2018 ◽  
Vol 548 ◽  
pp. 50-54
Author(s):  
Mohammad Bagheri ◽  
Rahim Faez
2017 ◽  
Vol 31 (12) ◽  
pp. 1750137 ◽  
Author(s):  
Shi-Quan Feng ◽  
Yang Yang ◽  
Jun-Yu Li ◽  
Xiao-Xu Jiang ◽  
Hai-Ning Li ◽  
...  

In this paper, we employed first-principle calculations to investigate the elastic properties, electronic properties and hardness of diamond and hexagonal W2B5 compounds under high pressure. The elastic properties were carried out to discuss the structural stability and the bond components of diamond and hexagonal W2B5. The electronic properties were presented to analysis the change of the bond components for W2B5. In addition, the hardness of these two crystals under high pressure was calculated by a semi-empirical method considering the role of metallic components and the effect of pressure on the hardness of diamond and hexagonal W2B5 was discussed.


2008 ◽  
Vol 43 (4) ◽  
pp. 1022-1026 ◽  
Author(s):  
S. Benalia ◽  
M. Ameri ◽  
D. Rached ◽  
R. Khenata ◽  
M. Rabah ◽  
...  

2015 ◽  
Vol 33 (2) ◽  
pp. 251-258
Author(s):  
Bendouma Doumi ◽  
Allel Mokaddem ◽  
Mustapha Ishak-Boushaki ◽  
Miloud Boutaleb ◽  
Abdelkader Tadjer

AbstractIn the present work, we have investigated the structural and electronic properties of TMAl (TM = Fe, Co, and Ni) transition metal aluminides in the B2 structure, using first-principle calculations of the density functional theory (DFT) based on the linearized augmented plane wave method (FP-LAPW) as implemented in the WIEN2k code, in which the energy of exchange and correlation are treated by the generalized gradient approximation (GGA), proposed in 1996 by Perdew, Burke and Ernzerhof (PBE). The ground state properties have been calculated and compared with other calculations, and the electronic structures of all FeAl, CoAl, and NiAl compounds exhibited a metallic behavior. It was depicted that the density of states is characterized by the large hybridization between the s-p (Al) and 3d (Fe, Co, and Ni) states, which creates the pseudogap in the region of anti-bonding states. Moreover, the band structures of FeAl, CoAl, and NiAl are similar to each other and the difference between them is in the energy level of each band relative to the Fermi level.


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