Monte Carlo simulation of low-noise avalanche photodiodes with heterojunctions

2002 ◽  
Vol 92 (8) ◽  
pp. 4791-4795 ◽  
Author(s):  
F. Ma ◽  
S. Wang ◽  
X. Li ◽  
K. A. Anselm ◽  
X. G. Zheng ◽  
...  
2012 ◽  
Vol 48 (4) ◽  
pp. 528-532 ◽  
Author(s):  
Wenlu Sun ◽  
Xiaoguang Zheng ◽  
Zhiwen Lu ◽  
Joe C. Campbell

2011 ◽  
Vol 23 (3) ◽  
pp. 030606 ◽  
Author(s):  
Gregg A. Radtke ◽  
Nicolas G. Hadjiconstantinou ◽  
Wolfgang Wagner

2011 ◽  
Vol 47 (12) ◽  
pp. 1531-1536 ◽  
Author(s):  
Wenlu Sun ◽  
Xiaoguang Zheng ◽  
Zhiwen Lu ◽  
Joe C. Campbell

2019 ◽  
Vol 301 ◽  
pp. 113699
Author(s):  
Chengcheng Zhao ◽  
Jianliang Huang ◽  
Yanhua Zhang ◽  
Wenjun Huang ◽  
Biyin Nie ◽  
...  

Author(s):  
Ryuichi Shimizu ◽  
Ze-Jun Ding

Monte Carlo simulation has been becoming most powerful tool to describe the electron scattering in solids, leading to more comprehensive understanding of the complicated mechanism of generation of various types of signals for microbeam analysis.The present paper proposes a practical model for the Monte Carlo simulation of scattering processes of a penetrating electron and the generation of the slow secondaries in solids. The model is based on the combined use of Gryzinski’s inner-shell electron excitation function and the dielectric function for taking into account the valence electron contribution in inelastic scattering processes, while the cross-sections derived by partial wave expansion method are used for describing elastic scattering processes. An improvement of the use of this elastic scattering cross-section can be seen in the success to describe the anisotropy of angular distribution of elastically backscattered electrons from Au in low energy region, shown in Fig.l. Fig.l(a) shows the elastic cross-sections of 600 eV electron for single Au-atom, clearly indicating that the angular distribution is no more smooth as expected from Rutherford scattering formula, but has the socalled lobes appearing at the large scattering angle.


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