Impact ionization coefficients and critical electric field in GaN

2021 ◽  
Vol 129 (18) ◽  
pp. 185702
Author(s):  
Takuya Maeda ◽  
Tetsuo Narita ◽  
Shinji Yamada ◽  
Tetsu Kachi ◽  
Tsunenobu Kimoto ◽  
...  
2020 ◽  
Vol 92 (1) ◽  
pp. 10301
Author(s):  
Tat Lung Wesley Ooi ◽  
Pei Ling Cheang ◽  
Ah Heng You ◽  
Yee Kit Chan

In this work, Monte Carlo model is developed to investigate the avalanche characteristics of GaN and Al0.45Ga0.55N avalanche photodiodes (APDs) using random ionization path lengths incorporating dead space effect. The simulation includes the impact ionization coefficients, multiplication gain and excess noise factor for electron- and hole-initiated multiplication with a range of thin multiplication widths. The impact ionization coefficient for GaN is higher than that of Al0.45Ga0.55N. For GaN, electron dominates the impact ionization at high electric field while hole dominate at low electric field whereas Al0.45Ga0.55N has hole dominate the impact ionization at higher field while electron dominate the lower field. In GaN APDs, electron-initiated multiplication is leading the multiplication gain at thinner multiplication widths while hole-initiated multiplication leads for longer widths. However for Al0.45Ga0.55N APDs, hole-initiated multiplication leads the multiplication gain for all multiplication widths simulated. The excess noise of electron-initiated multiplication in GaN APDs increases as multiplication widths increases while the excess noise decreases as the multiplication widths increases for hole-initiated multiplication. As for Al0.45Ga0.55N APDs, the excess noise for hole-initiated multiplication increases when multiplication width increases while the electron-initiated multiplication increases with the same gradient at all multiplication widths.


2012 ◽  
Vol 717-720 ◽  
pp. 545-548 ◽  
Author(s):  
D.M. Nguyen ◽  
Christophe Raynaud ◽  
Mihai Lazar ◽  
Gontran Pâques ◽  
Sigo Scharnholz ◽  
...  

Optical Beam Induced Current (OBIC) measurements have been performed on 4H-SiC avalanche diodes with very thin and highly doped avalanche region. The light source used in this study is an Ar-laser with a wavelength of 351 nm which results in a mixed carrier injection. From these measurements, impact ionization coefficients for 4H-SiC have been extracted in the electric field range from 3 to 4.8 MV/cm. In combination with ionization coefficients in our previous paper extracted from diodes with lowly doped avalanche region, we propose a set of parameters of impact ionization coefficients for 4H-SiC, applicable to a wide electric field range.


1993 ◽  
Vol 74 (1) ◽  
pp. 635-638
Author(s):  
H. Luquet ◽  
L. Gouskov ◽  
M. Pérotin ◽  
M. Karim ◽  
A. Rmou ◽  
...  

Author(s):  
Harry I. J. Lewis ◽  
Liang Qiao ◽  
Jeng Shiuh Cheong ◽  
Aina N. A. P. Baharuddin ◽  
Andrey B. Krysa ◽  
...  

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 ◽  
...  

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.


1995 ◽  
Vol 66 (2) ◽  
pp. 204-205 ◽  
Author(s):  
J. Lee ◽  
A. L. Gutierrez‐Aitken ◽  
S. H. Li ◽  
P. K. Bhattacharya

2010 ◽  
Vol 18 (3) ◽  
Author(s):  
S.G. Gasan-Zade ◽  
M.V. Strikha ◽  
G.A. Shepelskii

AbstractThe intensive far infra-red irradiation in the range of 80–100 μm was observed in uniaxially strained gapless p-Hg1−xCdxTe (MCT) with x = 0.14 in the strong electric field. The inverse occupation in strained MCT is created because the hot electrons distribution occurs in the c-band under impact ionization, while the holes are localized near the v-band top. The probability of band-to-band radiative transition increases dramatically when the acceptor level becomes resonance in the v-band. At threshold values of strain and electric field (P = 2.5–2.7 kbar, E = 50–55 V/cm), increase in irradiation (by 3 orders of magnitude) and increase in current (by 4–6 times) occur.


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