2019
DOI: 10.1109/ted.2019.2900743
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A New Expression for the Gain-Noise Relation of Single-Carrier Avalanche Photodiodes With Arbitrary Staircase Multiplication Regions

Abstract: We propose a simple expression to relate the total excess noise factor of a single carrier multiplication staircase avalanche photodiode to the excess noise factor and gain given by the individual conduction band discontinuities. The formula is valid when electron impact ionization dominates hole impact ionization; hence, it is especially suited for staircase APDs with In-rich multiplication regions, as opposed, for example, to GaAs/AlGaAs systems where hole ionization plays an important role. The formula has … Show more

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Cited by 3 publications
(3 citation statements)
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“…When P e tends to 1 (we double the electrons after each conduction band discontinuity), the excess noise factor tends to 1. A generalization of Eqs 18, 19 for a structure with non-uniform steps has been proposed in [30].…”
Section: Gain and Noise In Staircase Apdsmentioning
confidence: 99%
See 1 more Smart Citation
“…When P e tends to 1 (we double the electrons after each conduction band discontinuity), the excess noise factor tends to 1. A generalization of Eqs 18, 19 for a structure with non-uniform steps has been proposed in [30].…”
Section: Gain and Noise In Staircase Apdsmentioning
confidence: 99%
“…When dealing with X-rays, instead, the fact that one photon generates many e-h pairs can be interpreted as an additional multiplication step at the beginning of the structure having gain N = E ph /E ehp and excess noise factor F p = 1 + f/N. By employing the formula proposed in [30] to combine the multiplication steps, one find that for X-rays the current noise has a Power Spectral Density:…”
Section: Improved Random-path-length Algorithm For Time Response To S...mentioning
confidence: 99%
“…The capability of these models to represent the spatial distribution of ionisation path length generated by the analytical-band MC model [1] is presented for only one PDF of electron ionisation path length in GaAs at the electric field of 960 kVcm −1 . Recently, this simple RPL model has been improved and demonstrated capable of modelling avalanche characteristics in separate absorption and multiplication avalanche photodiodes (SAM-APDs) [12] and staircase APDs [13,14]. This improved RPL is based on a nonlocal historydependent model [15,16], where the electron and hole ionisation coefficients at a given position in the multiplication region do not depend on the local electric field, but on the whole electric field profile experienced by the carrier [17].…”
Section: Introductionmentioning
confidence: 99%