| Autor: |
Ramaswami, Kieran O, Curry, Richard J, Hinder, Ian, Johanson, Robert E, Kasap, Safa O |
| Předmět: |
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| Zdroj: |
Journal of Physics D: Applied Physics; 8/24/2022, Vol. 55 Issue 34, p1-17, 17p |
| Abstrakt: |
Charge collection efficiency (CE) η 0 under small signal conditions, corresponding to a uniform field in the detector medium, has been widely used in evaluating the performance of photoconductive detectors. The present paper answers the question, †What is the variance of the collected charge in an integrating detector as a function of photoinjection level and what are the errors if we continue to use the small signal equations? ’ The variance Ď 0 2 in η 0 under small signals has been theoretically derived in the literature and has been a key factor in the detective quantum efficiency modeling of integrating detectors based on various semiconductors. Ď 0 2 is a noise source and can degrade the detector performance under incomplete charge collection. The statistical variance Ď 0 2 in the CE η 0, under small signals and the variance Ď r 2 in the CE ηr under an arbitrary injection level r (injected charge divided by charge on the electrodes) have been studied using the Monte Carlo simulation model developed in this work to evaluate the difference between Ď r 2 and Ď 0 2 from small to large signals. Initial injection of electron and hole pairs and their subsequent transport and trapping in the presence of an electric field, which is calculated from the Poisson equation, is used to calculate the photocurrent. Each injected carrier is tracked as it moves in the semiconductor until it is either trapped or reaches the collection electrode. Trapped carriers do not contribute to the photocurrent but continue to contribute to the field through the Poisson equation. The instantaneous photocurrent i ph(t) is calculated from the drift of the free carriers through the Shockleyâ€"Ramo theorem. i ph(t) is integrated over the duration of the photocurrent to calculate the total collected charge and hence the CE ηr. The variance Ď r 2 in ηr is found from multiple simulations of ηr. The ηr and Ď r 2 have been generated over varying charge injection ratios r, the electron and hole ranges ÎĽĎ„, mean photoinjection depths δ and drift mobility ratios b. At full injection, the deviation Î" Ď r 2 of the CE variance Ď r 2 from the uniform field case Ď 0 2 ( i. e. Î" Ď r 2 = Ď r 2 â' Ď 0 2) may be as much as 40% larger or 20% lower than the small signal model prediction. This study provides the extent of errors involved in the variance of the CE in non-uniform fields and quantifies the increase in errors that can occur in high injection cases. In practice, typical injection ratios are less than 0.2, which means that the magnitude of percentage error Î" Ď r 2 / Ď 0 2 is less than 5%. [ABSTRACT FROM AUTHOR] |
| Databáze: |
Complementary Index |
| Externí odkaz: |
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