2008
DOI: 10.1063/1.2968434
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A simple method to characterize the afterpulsing effect in single photon avalanche photodiode

Abstract: A simple method is introduced for studying the afterpulsing effect in InGaAs single photon avalanche photodiode. The afterpulsing probability is obtained through measuring the detection efficiencies of various biasing pulses, while the incident photons are kept constant. The effect of excess bias and temperature on the afterpulsing probability is investigated. When the device temperature is higher than 170 K, the afterpulsing probability is lower than 5% for all excess bias voltages because the trapped carrier… Show more

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Cited by 12 publications
(7 citation statements)
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“…The characteristic decay of the afterpulse probability was sometimes thought to depend on the deep level in which the charge is trapped. Initial models 10 , 16 , 18 , 22 , 23 considered the decay from several distinct deep levels and proposed the “multiple exponential model” where the afterpulsing probability ( P exp ( t )) at a time t is given by: where τ k and A k is the de-trapping lifetime and amplitude factor for the k th deep level, and d is the offset due to noise counts.…”
Section: Canonical Models Of Afterpulsingmentioning
confidence: 99%
“…The characteristic decay of the afterpulse probability was sometimes thought to depend on the deep level in which the charge is trapped. Initial models 10 , 16 , 18 , 22 , 23 considered the decay from several distinct deep levels and proposed the “multiple exponential model” where the afterpulsing probability ( P exp ( t )) at a time t is given by: where τ k and A k is the de-trapping lifetime and amplitude factor for the k th deep level, and d is the offset due to noise counts.…”
Section: Canonical Models Of Afterpulsingmentioning
confidence: 99%
“…Recently, different fitting methods have been studied that employ a broad distribution of different exponential components instead of summating a few dominant discrete ones [26,27]. So far, most studies on the afterpulsing effect just have focused on its time-dependent probability distribution ignited by a single light pulse and do not discriminate the situation of a single ignition avalanche from that with multiple avalanches [12,[28][29][30][31]. However, this is not the real situation when the SPAD works continuously for photon detection.…”
Section: A Trapped Carriers and Afterpulsingmentioning
confidence: 99%
“…This is achieved using avalanche multiplication of photon-excited carriers, when they are biased above their breakdown voltage. These avalanches (breakdown events) produce large enough currents that can be registered employing low-power electronic discriminators [9]. APDs can be operated either in free-running mode or in gated mode [10].…”
Section: Introductionmentioning
confidence: 99%
“…Afterpulsing is a complex stochastic self-interacting phenomenon, which is proportional to the incoming light intensity. A number of techniques have been used to study it, including: time interval analysis [47][48][49], double gate method [14,50,51], temporal distribution (background decay) [37,52,53], in-gate effect of afterpulsing [9,10,31], corrections in g (2) (τ) correlation measurements [23,30,54,55], modified double-gate method (in order to study higher-order afterpulsing) [10,56], and other studies of the dependence of afterpulsing on operation settings [11,22].…”
Section: Introductionmentioning
confidence: 99%