2006
DOI: 10.1109/tim.2006.884291
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Dark Current and Signal-to-Noise Ratio in BDJ Image Sensors

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Cited by 5 publications
(16 citation statements)
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“…Almost all these charges contribute to the photocurrent without being affected by electronhole recombination, which is a much slower process. The drift current can thus be calculated by integrating the generation rate over the depletion layer [3, 4, 7, 10, 11, 19, 20, 22, 24, 26, 40, 43]: IdrθqAjnormalΦtexp(αWθ)where q is the elementary charge; A j is the active surface area; θ = 1 or 2 depending on the considered current and W 1 and W 2 denote the depletion-layer widths.…”
Section: The Bdj Photodetector Devicementioning
confidence: 99%
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“…Almost all these charges contribute to the photocurrent without being affected by electronhole recombination, which is a much slower process. The drift current can thus be calculated by integrating the generation rate over the depletion layer [3, 4, 7, 10, 11, 19, 20, 22, 24, 26, 40, 43]: IdrθqAjnormalΦtexp(αWθ)where q is the elementary charge; A j is the active surface area; θ = 1 or 2 depending on the considered current and W 1 and W 2 denote the depletion-layer widths.…”
Section: The Bdj Photodetector Devicementioning
confidence: 99%
“…Due to the recombination, only photo-generated carriers within a diffusion length from the depletion border can be collected and they contribute to the photocurrent. To determine the diffusion currents inside the BDJ detector, the concentration of excess minority carriers should first be calculated by solving the continuity equation with appropriate boundary conditions [3, 4, 7, 10, 11, 19, 20, 24, 26, 40, 43]. Diffusion component can then be determined for any kind of layer by: IphD=qAjDppnx|x orIphD=qAjDnnpx|xwhere D p and D n represent the diffusion coefficient for holes and electrons respectively; p n and n p represent the concentration of excess minority carriers in the observed quasi-neutral region.…”
Section: The Bdj Photodetector Devicementioning
confidence: 99%
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