scholarly journals Prediction of low energy phase transition in metal doped MoTe 2 from first principle calculations

2019 ◽  
Vol 125 (20) ◽  
pp. 204303
Author(s):  
Abhinav Kumar ◽  
Alejandro Strachan ◽  
Nicolas Onofrio
2012 ◽  
Vol 465 ◽  
pp. 33-36
Author(s):  
Zhi Dong Lin ◽  
Wen Long Song ◽  
Ju Cheng Zheng

The band structure and density of states (DOS) of Ti1-xSnxO2 solid solutions with x=0, 1/8, 1/4, 1/2 and 1 were investigated by means of the first-principle calculations based on density functional theory. The result indicated that band gap and Fermi level of TiO2-SnO2 vary continuously from those of pure TiO2 to those of Sn content increasing. In addition, the DOS moves towards low energy and the bang gap is broadened with growing value of x. The wide band gap and the low density of the states in the conduction band result in the enhancement of photoactivity in Ti1-xSnxO2.


2007 ◽  
Vol 392 (1-2) ◽  
pp. 229-232 ◽  
Author(s):  
Ye Deng ◽  
Ou-He Jia ◽  
Xiang-Rong Chen ◽  
Jun Zhu

2015 ◽  
Vol 17 (6) ◽  
pp. 4434-4440 ◽  
Author(s):  
Dawei Zhou ◽  
Chunying Pu ◽  
Chaozheng He ◽  
Feiwu Zhang ◽  
Cheng Lu ◽  
...  

The structure evolutions of BiOF under pressure are directly illustrated in our work by means of first principle calculations.


2011 ◽  
Vol 115 (19) ◽  
pp. 4976-4987 ◽  
Author(s):  
Michelle Morton ◽  
Joseph Barron ◽  
Travis Kemper ◽  
Susan Sinnott ◽  
Nedialka Iordanova

Materials ◽  
2019 ◽  
Vol 12 (21) ◽  
pp. 3612 ◽  
Author(s):  
Jianhui Yang ◽  
Qiang Fan ◽  
Bing Xiao ◽  
Yingchun Ding

A pressure-induced structural transition from the layered-like phase (Pnma) to another bilayer structure (Cmcm) in GeSe was investigated with first principle calculations. The variations of the structural, electronic, elastic, and vibrational properties of GeSe with the application of pressure were obtained. The transformation from the Pnma to Cmcm phase occurred at 34 GPa. The Cmcm phase structure showed dynamical stability above 37 GPa. The lattice parameters and the equation of state varied continuously at the transition pressure. Obvious stiffening in the C33 and C23 elastic constants associated with the compressive and shear components was observed to occur within the phase transition process. Two characteristic Raman modes (Ag and B3g) of the Pnma phase showed significant softening by increasing the pressure.


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