2018
DOI: 10.5334/jors.212
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Simple Monte Carlo Simulator for Modelling Linear Mode and Geiger Mode Avalanche Photodiodes in C++

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Cited by 6 publications
(5 citation statements)
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“…Our model relies on the following proposition: a process defined by the SDE ( 6) or (7) has a probability density function, as defined in (5), that is a solution of the PDE defining the generalized drift-diffusion (3). Proof of this statement and of existence of such density function can be found in [19].…”
Section: Transport Modelmentioning
confidence: 99%
See 1 more Smart Citation
“…Our model relies on the following proposition: a process defined by the SDE ( 6) or (7) has a probability density function, as defined in (5), that is a solution of the PDE defining the generalized drift-diffusion (3). Proof of this statement and of existence of such density function can be found in [19].…”
Section: Transport Modelmentioning
confidence: 99%
“…A great deal of effort has already been dedicated to finding accurate methods to simulate the SPAD operation and to extract reliable electrical characteristics of a given device architecture without the need of expensive and timeconsuming manufacturing and characterization. The state-ofthe-art methodologies rely on solving the Boltzmann transport equation (BTE) by means of particle Monte Carlo simulation in the phase-space, either under frozen field to investigate the details of avalanche process [5], [6] or self-consistently coupled to Poisson's equation to study all stages of SPAD operation [7]. This stochastic approach of transport can reproduce the statistical behavior of the SPAD, but it is known to be computationally very intensive, which makes it unsuitable for SPADs with sizes of several micrometers.…”
Section: Introductionmentioning
confidence: 99%
“…For the sake of comparison, the multiplication factors for the same reverse bias values have been calculated also by the Simple Monte Carlo v1.11 (SMC, [19]) code originally developed to simulate single photon avalanche diodes and that uses a simplified band structure to reduce computational requirements. The parameters assumed by the simulator to solve the Poisson equation are specified in Section II.E.…”
Section: A Modeling the Impact Ionizationmentioning
confidence: 99%
“…All, except [18], were validated against only a single In 0.53 Ga 0.47 As/InP APD design. A Simple Monte Carlo (SMC) model for the impact ionization process, first reported in 1999 [19], has recently been made available [20], with parameter files published for a range of avalanche materials including Si [21]. The SMC model is far less computationally intensive compared to Analytical and Full Band Monte Carlo models [22], [23], whilst incorporating sufficient impact ionization statistics (including dead space effects) to simulate a wide range of APD/SPAD designs, e.g., with thin avalanche regions and/or rapidly varying electric field profiles.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper we present an SMC parameter set for InP at 150 to 300 K, for use with our SMC simulator [20]. We comprehensively validated against a range of experimental data, including material characteristics such as saturation velocities, impact ionization coefficients for electrons and holes (α and β), as well as device characteristics such as M(V) and F(M) from multiple APD structures.…”
Section: Introductionmentioning
confidence: 99%