A formalism for the indirect Auger effect. I

A general formalism has been developed for the calculation of band-band Auger recombination and impact ionization rates in diamond and zinc blende type structures. The energy gap involved in the transition must be of order 1eV or greater, at room temperature, for direct gaps but is arbi­trary for indirect gaps. A recombination coefficient of 28.1 x 10 -32 cm 6 s -1 for GaP (hole-hole-electron collision) has been obtained in reasonable agreement with experiment. The formalism gives better theoretical values for Ge and Si than so far available. This has tended to reduce the recombination rates expected theoretically.

2001 ◽  
Vol 677 ◽  
Author(s):  
S. Picozzi ◽  
A. Continenza ◽  
R. Asahi ◽  
W. Mannstadt ◽  
C. B. Geller ◽  
...  

ABSTRACTWe present a method to calculate impact ionization and Auger recombination rates within density functional theory and a screened-exchange approach and implement it in the all- electron FLAPW method. We investigate the dependence of the overlap matrix elements as a function of the states involved along the main symmetry lines of the Brillouin zone. Our results for the final impact ionization rates along the main symmetry lines of the Brillouin zone. Our results for the final impact ionization rates along τ — X and τ —L directions for GaAs show a strong anisotropy imposed by energy and momentum conservation and related to the use of a realistic and accurate sX-LDA band structure.


The Auger recombination rate in indirect semiconductors with zincblende and diamond lattices is investigated, account being taken, for the first time, the properties of overlap integrals near symmetry points and axes. The effect of using theoretically estimated parameters is a reduction of the recombination coefficient by a factor 10. It is explained that the results, and those of the preceding paper, are still subject to uncertainties arising from the band structure so that only the order of magnitude of these coefficients can so far be regarded as known theoretically.


2010 ◽  
Vol 114 (39) ◽  
pp. 16860-16860
Author(s):  
Y. Fu ◽  
Y.-H. Zhou ◽  
Haibin Su ◽  
F. Y. C. Boey ◽  
H. Ågren

2010 ◽  
Vol 114 (9) ◽  
pp. 3743-3747 ◽  
Author(s):  
Y. Fu ◽  
Y.-H. Zhou ◽  
Haibin Su ◽  
F. Y. C. Boey ◽  
H. Ågren

1996 ◽  
Vol 423 ◽  
Author(s):  
J. Kolnik ◽  
I. H. Oguzman ◽  
K. F. Brennan ◽  
R. Wang ◽  
P. P. Ruden

AbstractIn this paper, we present the first calculations of the electron and hole initiated interband impact ionization rate in zinc blende phase GaN as a function of the applied electric field strength. The calculations are performed using an ensemble Monte Carlo simulator including the full details of the conduction and valence bands along with a numerically determined, wave-vector dependent interband ionization transition rate determined from an empirical pseudopotential calculation. The first four conduction bands and first three valence bands, which fully comprise the energy range of interest for device simulation, are included in the analysis. It is found that the electron and hole ionization rates are comparable over the full range of applied electric field strengths examined. Based on these calculations an avalanche photodiode, APD, made from bulk zinc blende GaN then would exhibit poor noise and bandwidth performance. It should be noted however, that the accuracy of the band structure employed and the scattering rates is presently unknown since little experimental information is available for comparison. Therefore, due to these uncertainties, it is difficult to unequivocally conclude that the ionization rates are comparable.


1982 ◽  
Vol 18 (14) ◽  
pp. 595 ◽  
Author(s):  
C.B. Su ◽  
J. Schlafer ◽  
J. Manning ◽  
R. Olshansky

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