2018
DOI: 10.1109/tns.2017.2778760
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Total-Ionizing Dose Effects on Charge Transfer Efficiency and Image Lag in Pinned Photodiode CMOS Image Sensors

Abstract: The total-ionizing dose (TID) effects on image lag in pinned photodiode CMOS image sensors are investigated thanks to various device variants in order to isolate the major radiationinduced effects on the charge transfer. It is shown that the main cause of the charge transfer degradation is the radiation-induced defects generation in the premetal dielectric (PMD) and in the transfer gate (TG) spacer vicinity which modifies the potential diagram at the photodiode/TG interface by the creation of a potential pocke… Show more

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Cited by 12 publications
(4 citation statements)
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References 18 publications
(25 reference statements)
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“…In PPD CISs, photo-generated carriers collected in the PPD are not completely transferred to the SN even in non-irradiated sensors. Incomplete charge transfer happens due to several reasons: long diffusion time in the PPD, potential barrier or pocket at the PPD-TG edge, charge trapping under the TG and charge spill-back from the SN to the PPD [27], [28]. Image lag was measured as the signal in the first sensor readout in darkness following illumination at a defined level in the previous image.…”
Section: Image Lagmentioning
confidence: 99%
“…In PPD CISs, photo-generated carriers collected in the PPD are not completely transferred to the SN even in non-irradiated sensors. Incomplete charge transfer happens due to several reasons: long diffusion time in the PPD, potential barrier or pocket at the PPD-TG edge, charge trapping under the TG and charge spill-back from the SN to the PPD [27], [28]. Image lag was measured as the signal in the first sensor readout in darkness following illumination at a defined level in the previous image.…”
Section: Image Lagmentioning
confidence: 99%
“…While CMOS image sensing technology is revolutionizing the digital imaging by shrinking the pixel pitch [39], one of the major challenges includes reducing image noise at the time of acquisition [40]. In the case of CMOS imaging sensors, main sources of noise include sensor electronics and photon starvation.…”
Section: Cmos Imaging and Sources Of Noisementioning
confidence: 99%
“…However, CMOS image sensors in star sensors are subject to cumulative effects and single-event transients by the widespread presence of protons in space. The cumulative effects cause the degradation of image sensor parameters such as dark current, uniformity, and full well capacity [6][7][8]. Moreover, protons can cause bulk defects inside the image sensor, resulting in hot pixels in the image.…”
Section: Introductionmentioning
confidence: 99%