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| 001 | 171758 | ||
| 005 | 20250129092510.0 | ||
| 024 | 7 | _ | |2 doi |a 10.1109/JSTQE.2014.2341562 |
| 024 | 7 | _ | |2 ISSN |a 1077-260X |
| 024 | 7 | _ | |2 ISSN |a 1558-4542 |
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| 037 | _ | _ | |a FZJ-2014-05324 |
| 041 | _ | _ | |a English |
| 082 | _ | _ | |a 530 |
| 100 | 1 | _ | |0 P:(DE-HGF)0 |a Bronzi, Danilo |b 0 |e Corresponding Author |
| 245 | _ | _ | |a 100 000 Frames/s 64 x 32 Single-Photon Detector Array for 2-D Imaging and 3-D Ranging |
| 260 | _ | _ | |a New York, NY |b IEEE |c 2014 |
| 336 | 7 | _ | |a Journal Article |b journal |m journal |0 PUB:(DE-HGF)16 |s 1421066161_25620 |2 PUB:(DE-HGF) |
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| 336 | 7 | _ | |a article |2 DRIVER |
| 520 | _ | _ | |a We report on the design and characterization of a multipurpose 64 × 32 CMOS single-photon avalanche diode (SPAD) array. The chip is fabricated in a high-voltage 0.35-μm CMOS technology and consists of 2048 pixels, each combining a very low noise (100 cps at 5-V excess bias) 30-μm SPAD, a prompt avalanche sensing circuit, and digital processing electronics. The array not only delivers two-dimensional intensity information through photon counting in either free-running (down to 10-μs integration time) or time-gated mode, but can also perform smart light demodulation with in-pixel background suppression. The latter feature enables phase-resolved imaging for extracting either three-dimensional depth-resolved images or decay lifetime maps, bymeasuring the phase shift between amodulated excitation light and the reflected photons. Pixel-level memories enable fully parallel processing and global-shutter readout, preventing motion artifacts (e.g., skew, wobble, motion blur) and partial exposure effects. The array is able to acquire very fast optical events at high frame-rate (up to 100 000 fps) and at single-photon level. Lownoise SPADs ensure high dynamic range (up to 110 dB at 100 fps) with peak photon detection efficiency of almost 50% at 410 nm. The SPAD imager provides different operating modes, thus, enabling both time-domain applications, like fluorescence lifetime imaging (FLIM) and fluorescence correlation spectroscopy, as well as frequency-domain FLIM and lock-in 3-D ranging for automotive vision and lidar. |
| 536 | _ | _ | |0 G:(DE-HGF)POF2-143 |a 143 - Radiation Research (POF2-143) |c POF2-143 |f POF II |x 0 |
| 536 | _ | _ | |0 G:(DE-HGF)POF2-434 |a 434 - Optics and Photonics (POF2-434) |c POF2-434 |f POF II |x 1 |
| 536 | _ | _ | |0 G:(DE-HGF)POF2-433 |a 433 - Process Development (POF2-433) |c POF2-433 |f POF II |x 2 |
| 536 | _ | _ | |0 G:(DE-HGF)POF2-472 |a 472 - Key Technologies and Innovation Processes (POF2-472) |c POF2-472 |f POF II |x 3 |
| 536 | _ | _ | |0 G:(DE-HGF)POF2-541 |a 541 - Photons (POF2-541) |c POF2-541 |f POF II |x 4 |
| 588 | _ | _ | |a Dataset connected to CrossRef, juser.fz-juelich.de |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Villa, Federica |b 1 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Tisa, Simone |b 2 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Tosi, Alberto |b 3 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Zappa, Franco |b 4 |
| 700 | 1 | _ | |0 P:(DE-Juel1)161528 |a Durini, Daniel |b 5 |u fzj |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Weyers, Sascha |b 6 |
| 700 | 1 | _ | |0 P:(DE-HGF)0 |a Brockherde, Werner |b 7 |
| 773 | _ | _ | |0 PERI:(DE-600)2025385-0 |a 10.1109/JSTQE.2014.2341562 |g Vol. 20, no. 6, p. 1 - 10 |n 6 |p 1 - 10 |t IEEE journal of selected topics in quantum electronics |v 20 |x 1558-4542 |y 2014 |
| 856 | 4 | _ | |u http://ieeexplore.ieee.org/xpl/abstractAuthors.jsp?arnumber=6872788 |
| 856 | 4 | _ | |u https://juser.fz-juelich.de/record/171758/files/FZJ-2014-05324.pdf |y Restricted |
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| 914 | 1 | _ | |y 2014 |
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