scholarly journals First Principles Studies on the Electronic Structure and Band Structure of Paraelectric SrTiO<sub>3</sub> by Different Approximations

2011 ◽  
Vol 02 (09) ◽  
pp. 934-943 ◽  
Author(s):  
H. Salehi
2009 ◽  
Vol 23 (19) ◽  
pp. 2339-2352 ◽  
Author(s):  
LI BIN SHI ◽  
SHUANG CHENG ◽  
RONG BING LI ◽  
LI KANG ◽  
JIAN WEI JIN ◽  
...  

Density of states and band structure of wurtzite ZnO are calculated by the CASTEP program based on density functional theory and plane-wave pseudopotential method. The calculations are carried out in axial and unaxial strains, respectively. The results of density of states in different strains show that the bottom of the conduction band is always dominated by Zn 4s, and the top of valence band is always dominated by O 2p. The variation of the band gap calculated from band structure is also discussed. In addition, p-d repulsion is used in investigating the variation of the top of the valence band in different strains and the results can be verified by electron density difference.


2019 ◽  
Vol 48 (5) ◽  
pp. 3059-3068 ◽  
Author(s):  
O. Y. Khyzhun ◽  
V. L. Bekenev ◽  
N. M. Denysyuk ◽  
L. I. Isaenko ◽  
A. P. Yelisseyev ◽  
...  

2011 ◽  
Vol 216 ◽  
pp. 341-344 ◽  
Author(s):  
Qi Jun Liu ◽  
Zheng Tang Liu ◽  
Li Ping Feng

Electronic structure, effective masses and optical properties of monoclinic HfO2were studied using the plane-wave ultrasoft pseudopotential technique based on the first-principles density-functional theory (DFT). The calculated equilibrium lattice parameters are in agreement with the previous works. From the band structure, the effective masses and optical properties are obtained. The calculated band structure shows that monoclinic HfO2has indirect band gap and all of the effective masses of electrons and holes are less than that of a free electron. The peaks position distributions of imaginary parts of the complex dielectric function have been explained according to the theory of crystal-field and molecular-orbital bonding.


1987 ◽  
Vol 99 ◽  
Author(s):  
D. A. Papaconstantopoulos ◽  
M. J. Deweert ◽  
W. E. Pickett

ABSTRACTWe have fit our first principles LAPW band structure results for the high Tc superconductor La2CuO4 to a tight-binding Hamiltonian that contains s, p, and d interactions from the three components of these materials. Our fit reproduces very accurately the 17 lower bands of this material and especially the Fermi surface.


2012 ◽  
Vol 1407 ◽  
Author(s):  
Paul Plachinda ◽  
Raj Solanki ◽  
David Evans

ABSTRACTWe have employed first-principles density-functional calculations to study the electronic characteristics of graphene functionalized by metal-bis-arene and metal-carbonyl molecules. It is shown that functionalization with M-bis-arene (M(C6H6)@gr, M=Ti, V, Cr, Mn, Fe) molecules leads to an opening in the band gap of graphene (up to 0.81eV for the Cr derivative), and functionalization with M-carbonyl (M(CX)3@gr, X=O,N; M= Cr, Mn, Fe, Co) up to one 1eV for M=Cr and X=O, and therefore transforms graphene from a semi-metal to a semiconductor. The band gap induced by attachment of a metal atom topped by a functionalizing group is attributed to modification of π-conjugation and depends on the concentration of functionalizing molecules, metal’s and moiety’s electronic structure. This approach offers a means of tailoring the band structure of graphene and potentially its applications for future electronic devices.


2017 ◽  
Vol 31 (12) ◽  
pp. 1750194 ◽  
Author(s):  
Zhi-Jie Fang ◽  
Xiao-Shuai Zhai ◽  
Zheng-Lin Li ◽  
Rong-Jun Pan ◽  
Man Mo

Using the first-principle methods, the pressure dependence of the electronic structure and band structure of kaolinite were studied within the local-density approximation. The calculated results show that pressure would chiefly alter the band structure of kaolinite, while pressure can have its main effect on the band gap of kaolinite. At p = 0.6 GPa, band structure of kaolinite first converts an indirect gap into a direct gap, and then recovers an indirect gap structure at p = 66.2 GPa because CBM shift in the band structure is under high-pressure. The bond Si–O is more stable than bond Al–O under pressure, in addition, pressure has a significant effect on the inner hydroxyl bond of kaolinite and leads to a large variation of H–O(inner) bond lengths. The calculated results will not only help to understand the electronic structure of kaolinite under pressure, but also provide theoretical guidance for deal with the safe problems of soft-rock tunnel engineering.


Sign in / Sign up

Export Citation Format

Share Document