Depth imaging through obscurants using time-correlated single-photon counting

Author(s):  
Frank Christnacher ◽  
Gerald S. Buller ◽  
Rachael Tobin ◽  
Abderrahim Halimi ◽  
Aongus McCarthy ◽  
...  
2015 ◽  
Vol 23 (26) ◽  
pp. 33911 ◽  
Author(s):  
Aurora Maccarone ◽  
Aongus McCarthy ◽  
Ximing Ren ◽  
Ryan E. Warburton ◽  
Andy M. Wallace ◽  
...  

2012 ◽  
Author(s):  
Gerald S. Buller ◽  
Aongus McCarthy ◽  
Ximing Ren ◽  
Nathan R. Gemmell ◽  
Robert J. Collins ◽  
...  

2015 ◽  
Author(s):  
Aurora Maccarone ◽  
Aongus McCarthy ◽  
Ximing Ren ◽  
Ryan E. Warburton ◽  
Andy M. Wallace ◽  
...  

2010 ◽  
Author(s):  
Nils J. Krichel ◽  
Aongus McCarthy ◽  
Andrew M. Wallace ◽  
Jing Ye ◽  
Gerald S. Buller

2016 ◽  
Author(s):  
Aurora Maccarone ◽  
Aongus McCarthy ◽  
Abderrahim Halimi ◽  
Rachael Tobin ◽  
Andy M. Wallace ◽  
...  

Sensors ◽  
2021 ◽  
Vol 21 (14) ◽  
pp. 4850
Author(s):  
Aurora Maccarone ◽  
Giulia Acconcia ◽  
Ulrich Steinlehner ◽  
Ivan Labanca ◽  
Darryl Newborough ◽  
...  

We present an optical depth imaging system suitable for highly scattering underwater environments. The system used the time-correlated single-photon counting (TCSPC) technique and the time-of-flight approach to obtain depth profiles. The single-photon detection was provided by a linear array of single-photon avalanche diode (SPAD) detectors fabricated in a customized silicon fabrication technology for optimized efficiency, dark count rate, and jitter performance. The bi-static transceiver comprised a pulsed laser diode source with central wavelength 670 nm, a linear array of 16 × 1 Si-SPAD detectors, with a dedicated TCSPC acquisition module. Cylindrical lenses were used to collect the light scattered by the target and image it onto the sensor. These laboratory-based experiments demonstrated single-photon depth imaging at a range of 1.65 m in highly scattering conditions, equivalent up to 8.3 attenuation lengths between the system and the target, using average optical powers of up to 15 mW. The depth and spatial resolution of this sensor were investigated in different scattering conditions.


Author(s):  
Aurora Maccarone ◽  
Aongus McCarthy ◽  
Julian A. Tachella ◽  
Diego Aguirre Garcia ◽  
Francesco Mattioli Della Rocca ◽  
...  

2011 ◽  
Author(s):  
Gerald S. Buller ◽  
Nils J. Krichel ◽  
Aongus McCarthy ◽  
Nathan R. Gemmell ◽  
Michael G. Tanner ◽  
...  

Sensors ◽  
2018 ◽  
Vol 18 (11) ◽  
pp. 4016 ◽  
Author(s):  
Chao Zhang ◽  
Scott Lindner ◽  
Ivan Antolovic ◽  
Martin Wolf ◽  
Edoardo Charbon

Per-pixel time-to-digital converter (TDC) architectures have been exploited by single-photon avalanche diode (SPAD) sensors to achieve high photon throughput, but at the expense of fill factor, pixel pitch and readout efficiency. In contrast, TDC sharing architecture usually features high fill factor at small pixel pitch and energy efficient event-driven readout. While the photon throughput is not necessarily lower than that of per-pixel TDC architectures, since the throughput is not only decided by the TDC number but also the readout bandwidth. In this paper, a SPAD sensor with 32 × 32 pixels fabricated with a 180 nm CMOS image sensor technology is presented, where dynamically reallocating TDCs were implemented to achieve the same photon throughput as that of per-pixel TDCs. Each 4 TDCs are shared by 32 pixels via a collision detection bus, which enables a fill factor of 28% with a pixel pitch of 28.5 μm. The TDCs were characterized, obtaining the peak-to-peak differential and integral non-linearity of −0.07/+0.08 LSB and −0.38/+0.75 LSB, respectively. The sensor was demonstrated in a scanning light-detection-and-ranging (LiDAR) system equipped with an ultra-low power laser, achieving depth imaging up to 10 m at 6 frames/s with a resolution of 64 × 64 with 50 lux background light.


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