Comment on “Oxygen ionization rates at Mars and Venus: Relative contributions of impact ionization and charge exchange” by M. H. Zhang, J. G. Luhmann, A. F. Nagy, J. R. Spreiter, and S. S. Stahara

1996 ◽  
Vol 101 (E3) ◽  
pp. 7599-7602 ◽  
Author(s):  
A. M. Krymskii ◽  
T. K. Breus
Keyword(s):  
Charge Exchange ◽  
Impact Ionization ◽  
Oxygen Ionization ◽  
Ionization Rates

Oxygen ionization rates at Mars and Venus: Relative contributions of impact ionization and charge exchange

1993 ◽  
Vol 98 (E2) ◽  
pp. 3311-3318 ◽  
Author(s):  
M. H. G. Zhang ◽  
J. G. Luhmann ◽  
A. F. Nagy ◽  
J. R. Spreiter ◽  
S. S. Stahara
Keyword(s):  
Charge Exchange ◽  
Impact Ionization ◽  
Oxygen Ionization ◽  
Ionization Rates

Temperature Dependence of Hole Impact Ionization Coefficient in 4H-SiC Photodiodes

2009 ◽  
Vol 615-617 ◽  
pp. 311-314 ◽  
Author(s):  
W.S. Loh ◽  
J.P.R. David ◽  
B.K. Ng ◽  
Stanislav I. Soloviev ◽  
Peter M. Sandvik ◽  
...  
Keyword(s):  
Phonon Scattering ◽  
Impact Ionization ◽  
Positive Temperature Coefficient ◽  
Positive Temperature ◽  
Different Temperatures ◽  
Ionization Coefficients ◽  
Increasing Temperature ◽  
The Impact ◽  
Good Agreement ◽  
Ionization Rates

Hole initiated multiplication characteristics of 4H-SiC Separate Absorption and Multiplication Avalanche Photodiodes (SAM-APDs) with a n- multiplication layer of 2.7 µm were obtained using 325nm excitation at temperatures ranging from 300 to 450K. The breakdown voltages increased by 200mV/K over the investigated temperature range, which indicates a positive temperature coefficient. Local ionization coefficients, including the extracted temperature dependencies, were derived in the form of the Chynoweth expression and were used to predict the hole multiplication characteristics at different temperatures. Good agreement was obtained between the measured and the modeled multiplication using these ionization coefficients. The impact ionization coefficients decreased with increasing temperature, corresponding to an increase in breakdown voltage. This result agrees well with the multiplication characteristics and can be attributed to phonon scattering enhanced carrier cooling which has suppressed the ionization process at high temperatures. Hence, a much higher electric field is required to achieve the same ionization rates.

Measurement of the impact ionization rates in Al0.06Ga0.94Sb

1990 ◽  
Vol 57 (3) ◽  
pp. 249-251 ◽  
Author(s):  
H. Kuwatsuka ◽  
T. Mikawa ◽  
S. Miura ◽  
N. Yasuoka ◽  
Y. Kito ◽  
...  
Keyword(s):  
Impact Ionization ◽  
The Impact ◽  
Ionization Rates

Impact ionization rates for electrons and holes in GaAs1−xSbxalloys

1976 ◽  
Vol 28 (7) ◽  
pp. 403-405 ◽  
Author(s):  
T. P. Pearsall ◽  
R. E. Nahory ◽  
M. A. Pollack
Keyword(s):  
Impact Ionization ◽  
Ionization Rates

Comparison of Electron and Hole Initiated Impact Ionization in Zincblende and Wurtzite Phase Gallium Nitride

1997 ◽  
Vol 468 ◽  
Author(s):  
E. Bellotti ◽  
I. H. Oguzman ◽  
J. Kölnik ◽  
K. F. Brennan ◽  
R. Wang ◽  
...  
Keyword(s):  
Applied Field ◽  
Impact Ionization ◽  
Full Range ◽  
Wurtzite Phase ◽  
Valence Bands ◽  
Two Phases ◽  
Ionization Coefficients ◽  
Direct Numerical Integration ◽  
Applied Fields ◽  
Ionization Rates

ABSTRACTIn this paper, we present the first calculations of the electron and hole impact ionizatioi coefficients for both wurtzite and zincblende phase GaN as a function of the applied electrii field. The calculations are made using an ensemble Monte Carlo simulator including the ful details of the conduction and valence bands derived from an empirical pseudopotentia calculation. The interband impact ionization transition rates for both carrier species an determined by direct numerical integration including a wavevector dependent dielectric function It is found that the electron and hole ionization coefficients are comparable in zincblende Ga> at an applied field of ∼ 3 MV/cm, yet vary to a slight degree at both higher and lower applied field strengths. In the wurtzite phase, the electron and hole coefficients are comparable at hig] fields but diverge at lower applied fields. The most striking result is that the ionization rates an predicted to be substantially different for both carrier species between the two phases. It i predicted that the ionization rates for both carrier species in the zincblende phase are significanti; higher than in the wurtzite phase over the full range of applied fields examined.

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