Front and Back Illuminated Dynamic and Active Pixel Vision Sensors ...
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> REPLACE THIS LINE WITH YOUR PAPER IDENTIFICATION NUMBER (DOUBLE-CLICK HERE TO EDIT) REPLACE THIS LINE WITH YOUR PAPER IDENTIFICATION NUMBER (DOUBLE-CLICK HERE TO EDIT) REPLACE THIS LINE WITH YOUR PAPER IDENTIFICATION NUMBER (DOUBLE-CLICK HERE TO EDIT) 4 up to 1050nm. 2 LED: CREE MHDGWT-0000-000N0UK230GCT-ND White 3000K, http://www.cree.com/led-components/media/documents/ds-MHDG.pdf 3 Mitutoyo Xenon‐based white light source
Fig. 3 Quantum Efficiency spectrum of BSI DAVIS and FSI DAVIS; (inset) QE BSI/QE FSI DAVIS ratio spectrum, the color scale represents wavelength color.
Fig. 4 Average pixel leak activity frequency of BSI and FSI DAVIS, with and without 84714 NIR cut filter using Xenon light source.
B. Leak Activity (LA) LA was characterized in [14] by measuring average pixel frequency of leak events fpar due to parasitic photocurrent in Dr. In our previous characterizations, we mistakenly measured LA using white LED lighting2 which lacks NIR content. In order to investigate the effect of NIR light on the BSI DAVIS we repeated the measurements with an incandescent Xenon source light3 that has significant NIR content. During the experiments, the bias setting were left untouched. The bias currents Ioff < Id < Ion determine the event thresholds (Id = 40nA, Ion = 1.9uA, Ioff = 1.8nA), while the bias current IPr and IPrSF control the amplifiers in the first and second stage, determining the pixel bandwidth (IPr = 172pA, IPrSF = 5.3pA) [14]. After biasing BSI and FSI DAVIS
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