Calculated Valence-Band Densities of States and Photoemission Spectra of Diamond and Zinc-Blende Semiconductors

1973 ◽  
Vol 8 (6) ◽  
pp. 2786-2794 ◽  
Author(s):  
J. Chelikowsky ◽  
D. J. Chadi ◽  
Marvin L. Cohen
1995 ◽  
Vol 51 (15) ◽  
pp. 9497-9507 ◽  
Author(s):  
A. Stuck ◽  
J. Osterwalder ◽  
T. Greber ◽  
L. Schlapbach ◽  
R. C. Albers ◽  
...  

2005 ◽  
Vol 98 (1) ◽  
pp. 013704 ◽  
Author(s):  
L. Zhang ◽  
I. Konovalov ◽  
D. Wett ◽  
D. Schulze ◽  
R. Szargan ◽  
...  

1993 ◽  
Vol 297 ◽  
Author(s):  
JoŽE Furlan ◽  
Franc Smole ◽  
Pavle PopoviĆ

Effective densities of states in conduction and valence band, Nc and Nv, are usually set to a fixed value of 1019 to 1020 cm−3 in all computer simulations of a-Si structures. In this contribution the densities Nc and Nv are analytically expressed for different selected extended states distributions. The derivatives d(lnNc)/dx and d(lnNv)/dx, representing specific terms in transport equations, are expressed as function of position dependent band structure. The effect of an increased disorder in heterojunction is simulated by Gaussian distribution of states in a linearly graded heterojunction region.


1974 ◽  
Vol 9 (2) ◽  
pp. 600-621 ◽  
Author(s):  
L. Ley ◽  
R. A. Pollak ◽  
F. R. McFeely ◽  
S. P. Kowalczyk ◽  
D. A. Shirley

1990 ◽  
Vol 192 ◽  
Author(s):  
Samer Aljishi ◽  
J. David Cohen ◽  
Shu Jin ◽  
Lothar Ley

ABSTRACTThe energy distribution and temperature dependence of the conduction and valence band tail density of states in a-Si:H and a-Si,Ge:H alloys is determined via total yield photoelectron spectroscopy. All films are observed to possess purely exponential conduction and valence band tail densities of states; however, the characteristic energy of the conduction band tail increases much more rapidly with temperature in the range of 300K to 550K than that of the valence band tail. This indicates that over that temperature range the conduction band tail is considerably more susceptible to thermal disorder than to structural disorder whereas the reverse holds for the valence band tail.


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