A 240 × 160 3D-Stacked SPAD dToF Image Sensor With Rolling Shutter and In-Pixel Histogram for Mobile Devices
A 240 <inline-formula> <tex-math notation="LaTeX">\times </tex-math></inline-formula> 160 single-photon avalanche diode (SPAD) sensor integrated with a 3D-stacked 65nm/65nm CMOS technology is reported for direct time-of-flight (dToF) 3D imaging in mobile devices. Th...
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| Published in | IEEE open journal of solid-state circuits Vol. 2; pp. 3 - 11 |
|---|---|
| Main Authors | , , , , , , |
| Format | Journal Article |
| Language | English |
| Published |
New York
IEEE
2022
The Institute of Electrical and Electronics Engineers, Inc. (IEEE) |
| Subjects | |
| Online Access | Get full text |
| ISSN | 2644-1349 2644-1349 |
| DOI | 10.1109/OJSSCS.2021.3118332 |
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| Abstract | A 240 <inline-formula> <tex-math notation="LaTeX">\times </tex-math></inline-formula> 160 single-photon avalanche diode (SPAD) sensor integrated with a 3D-stacked 65nm/65nm CMOS technology is reported for direct time-of-flight (dToF) 3D imaging in mobile devices. The top tier is occupied by backside illuminated SPADs with 16 <inline-formula> <tex-math notation="LaTeX">\mu {\mathrm{ m}} </tex-math></inline-formula> pitch and 49.7% fill-factor. The SPADS consists of multiple 16<inline-formula> <tex-math notation="LaTeX">\times </tex-math></inline-formula>16 SPADs top groups, in which each of 8 <inline-formula> <tex-math notation="LaTeX">\times </tex-math></inline-formula> 8 SPADs sub-group shares a 10-bit, 97.65ps and 100ns range time-to-digital converter (TDC) in a quad-partition rolling shutter mode. During the exposure of each rolling stage, partial histogramming readout (PHR) approach is implemented to compress photon events to in-pixel histograms. Since the fine histograms is incomplete, for the first time we propose histogram distortion correction (HDC) algorithm to solve the linearity discontinuity at the coarse bin edges. With this algorithm, depth measurement up to 9.5m achieves an accuracy of 1cm and precision of 9mm in office lighting condition. Outdoor measurement with 10 klux sunlight achieves a maximum distance detection of 4m at 20 fps, using a VCSEL laser with the average power of 90 mW and peak power of 15 W. |
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| AbstractList | A 240 <tex-math notation="LaTeX">$\times$ </tex-math> 160 single-photon avalanche diode (SPAD) sensor integrated with a 3D-stacked 65nm/65nm CMOS technology is reported for direct time-of-flight (dToF) 3D imaging in mobile devices. The top tier is occupied by backside illuminated SPADs with 16 <tex-math notation="LaTeX">$\mu {\mathrm{ m}}$ </tex-math> pitch and 49.7% fill-factor. The SPADS consists of multiple 16 <tex-math notation="LaTeX">$\times$ </tex-math>16 SPADs top groups, in which each of 8 <tex-math notation="LaTeX">$\times$ </tex-math> 8 SPADs sub-group shares a 10-bit, 97.65ps and 100ns range time-to-digital converter (TDC) in a quad-partition rolling shutter mode. During the exposure of each rolling stage, partial histogramming readout (PHR) approach is implemented to compress photon events to in-pixel histograms. Since the fine histograms is incomplete, for the first time we propose histogram distortion correction (HDC) algorithm to solve the linearity discontinuity at the coarse bin edges. With this algorithm, depth measurement up to 9.5m achieves an accuracy of 1cm and precision of 9mm in office lighting condition. Outdoor measurement with 10 klux sunlight achieves a maximum distance detection of 4m at 20 fps, using a VCSEL laser with the average power of 90 mW and peak power of 15 W. A 240 <inline-formula> <tex-math notation="LaTeX">\times </tex-math></inline-formula> 160 single-photon avalanche diode (SPAD) sensor integrated with a 3D-stacked 65nm/65nm CMOS technology is reported for direct time-of-flight (dToF) 3D imaging in mobile devices. The top tier is occupied by backside illuminated SPADs with 16 <inline-formula> <tex-math notation="LaTeX">\mu {\mathrm{ m}} </tex-math></inline-formula> pitch and 49.7% fill-factor. The SPADS consists of multiple 16<inline-formula> <tex-math notation="LaTeX">\times </tex-math></inline-formula>16 SPADs top groups, in which each of 8 <inline-formula> <tex-math notation="LaTeX">\times </tex-math></inline-formula> 8 SPADs sub-group shares a 10-bit, 97.65ps and 100ns range time-to-digital converter (TDC) in a quad-partition rolling shutter mode. During the exposure of each rolling stage, partial histogramming readout (PHR) approach is implemented to compress photon events to in-pixel histograms. Since the fine histograms is incomplete, for the first time we propose histogram distortion correction (HDC) algorithm to solve the linearity discontinuity at the coarse bin edges. With this algorithm, depth measurement up to 9.5m achieves an accuracy of 1cm and precision of 9mm in office lighting condition. Outdoor measurement with 10 klux sunlight achieves a maximum distance detection of 4m at 20 fps, using a VCSEL laser with the average power of 90 mW and peak power of 15 W. A 240 [Formula Omitted] 160 single-photon avalanche diode (SPAD) sensor integrated with a 3D-stacked 65nm/65nm CMOS technology is reported for direct time-of-flight (dToF) 3D imaging in mobile devices. The top tier is occupied by backside illuminated SPADs with 16 [Formula Omitted] pitch and 49.7% fill-factor. The SPADS consists of multiple 16[Formula Omitted]16 SPADs top groups, in which each of 8 [Formula Omitted] 8 SPADs sub-group shares a 10-bit, 97.65ps and 100ns range time-to-digital converter (TDC) in a quad-partition rolling shutter mode. During the exposure of each rolling stage, partial histogramming readout (PHR) approach is implemented to compress photon events to in-pixel histograms. Since the fine histograms is incomplete, for the first time we propose histogram distortion correction (HDC) algorithm to solve the linearity discontinuity at the coarse bin edges. With this algorithm, depth measurement up to 9.5m achieves an accuracy of 1cm and precision of 9mm in office lighting condition. Outdoor measurement with 10 klux sunlight achieves a maximum distance detection of 4m at 20 fps, using a VCSEL laser with the average power of 90 mW and peak power of 15 W. |
| Author | Zang, Kai Jia, Jieyang Zhang, Chao Ma, Zhijie Wang, Letian Qin, Yu Zhang, Ning |
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| Cites_doi | 10.1109/LED.2017.2755989 10.1109/ISSCC.2015.7062997 10.1109/JSSC.2015.2467170 10.1109/JSSC.2013.2284352 10.1109/JSSC.2018.2883720 10.1109/JSSC.2019.2939083 10.1109/ISSCC.2018.8310201 10.1109/JSSC.2016.2623635 10.1109/JSSC.2018.2868315 10.1109/ISSCC42613.2021.9366010 10.1109/JSSC.2020.2970704 10.1109/IEDM.2016.7838372 10.1109/JSSC.2012.2227607 10.1109/JSTQE.2014.2342197 10.1109/ISSCC42613.2021.9365961 10.1109/ISSCC42613.2021.9366022 |
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| SubjectTerms | 3-D imaging 3-D stacking Algorithms Avalanche diodes Clocks CMOS Converters Depth measurement Electronic devices histogram Histograms image sensor LIDAR Photon avalanches Photonics Photons Pixels Power demand Single-photon avalanche diodes single-photon avalanche diodes (SPADs) Three-dimensional displays time-of-flight (dToF) time-to-digital converter (TDC) Vertical cavity surface emission lasers |
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| Title | A 240 × 160 3D-Stacked SPAD dToF Image Sensor With Rolling Shutter and In-Pixel Histogram for Mobile Devices |
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