scholarly journals EFFECTIVE QUASIPARTICLE RECOMBINATION TIMES AND ELECTRONIC DENSITY OF STATES AT THE FERMI LEVEL IN SUPERCONDUCTING FILMS

1978 ◽  
Vol 39 (C6) ◽  
pp. C6-515-C6-516 ◽  
Author(s):  
P. W. Epperlein ◽  
K. Laßmann ◽  
W. Eisenmenger
1993 ◽  
Vol 07 (07) ◽  
pp. 471-481 ◽  
Author(s):  
JIU-YUAN GE ◽  
YUN-SONG ZHOU ◽  
LI-YUAN ZHONG ◽  
HUAI-YU WANG

The electronic density of states (DOS) of both pure and Co-substituted YBa 2 Cu 3 O 7 has been calculated by a recursion method. The results show that the total DOS at the Fermi level of YBa 2 Cu 3 O 7 mainly comes from the contributions of the O 2p and Cu 3d orbitals. After Co doping, the O 2p–Cu 3d bonds are destroyed while the O 2p–Co 3d bonds are formed at lower energies, and the total DOS at the Fermi level decreases strikingly. In addition, our results reveal that the CuO chain has a one-dimensional feature.


2015 ◽  
Vol 713-715 ◽  
pp. 2966-2969
Author(s):  
Yue Fan ◽  
Shao Chang Chen

In this paper, we studied the electronic density of states (DOS) and optical properties ZnO using first-principles method. We find that the electronic density of states was different in bulk ZnO and ZnO nanotube. The DOS of bulk ZnO spread at wide energy while the DOS of ZnO nanotube concentrated in a narrow energy range. The peak around-18 eV moved to a higher energy. The peaks more than Fermi level concentrated to the Fermi level, which meant the conductivity of ZnO nanotube was better than that of bulk ZnO. We also calculated the optical properties of ZnO nanotube. The optical properties showed that there were peaks around 8 eV, which may come from electrons transition between Zn 3dand O 2pstates. Our calculation provided a reference for the application of ZnO nanotube in optical devices.


2003 ◽  
Vol 805 ◽  
Author(s):  
Y. Ishii ◽  
K. Nozawa ◽  
T. Fujiwara

ABSTRACTElectronic structures of hexagonal Zn-Mg-Y and Cd58Y13 compounds are studied by first-principles calculations. Both of the systems show deep pseudogap in the electronic density of states near the Fermi level and considered to be stabilized electronically. To illustrate bonding nature of electronic wavefunctions, the crystal orbital Hamilton population (COHP) is calculated for neighboring pairs of atoms in the unit cell. It is found that the bonding nature is changed from bonding to anti-bonding almost exactly at the Fermi level for Zn-Zn and Cd-Cd bonds. On the contrary, for Zn/Cd-Y bonds, both of the states below and above the pseudogap behave as bonding ones. Possible effects of the p-d hybridization are discussed.


2004 ◽  
Vol 241 (5) ◽  
pp. 1058-1065 ◽  
Author(s):  
M. Hidaka ◽  
N. Tokiwa ◽  
S. Takahashi ◽  
J.-Y. Choi ◽  
J. M. Lee

1992 ◽  
Vol 259 ◽  
Author(s):  
A. Hughes ◽  
T-H. Shen ◽  
C.C. Matthai

ABSTRACTThe electronic density of states (DOS) for the Si(111) (√3×√3)-Sb system has been calculated using the tight binding method in the Extended Hiickel Approximation. We find that there is a gap of about 0.8eV between the valence band maximum (VBM) and a surface state. This is in contrast with the case of the unreconstructed (lxl) surface where the Fermi level lies at the surface state.


2005 ◽  
Vol 242 (4) ◽  
pp. 899-908 ◽  
Author(s):  
M. Hidaka ◽  
M. Soejima ◽  
Y. Noguchi ◽  
M. Miyayama ◽  
Sun-Hee Choi ◽  
...  

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