TY - JOUR
T1 - A Programmable Active Recharge Circuit for SPAD in 110-nm BSI CMOS
AU - Moon, Hyunho
AU - Park, Byungchoul
AU - Kim, Hyeon June
N1 - Publisher Copyright:
© 2013 IEEE.
PY - 2025
Y1 - 2025
N2 - This paper presents a programmable active recharge (AR) circuit optimized for a single-photon avalanche diode (SPAD) fabricated in a 110-nm BSI CMOS process. The SPAD employs a p-well and deep n-well junction. A retrograde p-substrate guard-ring, which is located at the junction edges, suppresses the premature breakdown of the SPAD. An NMOS recharge transistor is connected to the SPAD anode and is driven by an active recharge signal (ΦAR), which is generated by the AR circuit. The AR circuit consists of an NMOS recharge transistor (MAR), a current-starved inverter chain, and an AND gate, which detects the SPAD pulse and recharges the SPAD for the consecutive photon detection. By controlling the bias of the inverter chain, the delay and pulse width of ΦAR (DEL and WID) can be externally controlled. To optimize the timing of the AR circuit, an afterpulsing probability (APP) is characterized using inter-avalanche histogramming technique. The APP is measured at 0.1% with an interval range of 20 μs. When adjusting the delay of ΦAR, the number of irregular peaks within the first 2 ns time interval are increased by a factor of 3.2. In contrast, varying the pulse width of ΦAR shows no significant correlation with the number of irregular peaks. These results demonstrate that the delay of ΦAR should be controlled precisely for minimizing APP and improving the SPAD performance in high-speed photon counting applications.
AB - This paper presents a programmable active recharge (AR) circuit optimized for a single-photon avalanche diode (SPAD) fabricated in a 110-nm BSI CMOS process. The SPAD employs a p-well and deep n-well junction. A retrograde p-substrate guard-ring, which is located at the junction edges, suppresses the premature breakdown of the SPAD. An NMOS recharge transistor is connected to the SPAD anode and is driven by an active recharge signal (ΦAR), which is generated by the AR circuit. The AR circuit consists of an NMOS recharge transistor (MAR), a current-starved inverter chain, and an AND gate, which detects the SPAD pulse and recharges the SPAD for the consecutive photon detection. By controlling the bias of the inverter chain, the delay and pulse width of ΦAR (DEL and WID) can be externally controlled. To optimize the timing of the AR circuit, an afterpulsing probability (APP) is characterized using inter-avalanche histogramming technique. The APP is measured at 0.1% with an interval range of 20 μs. When adjusting the delay of ΦAR, the number of irregular peaks within the first 2 ns time interval are increased by a factor of 3.2. In contrast, varying the pulse width of ΦAR shows no significant correlation with the number of irregular peaks. These results demonstrate that the delay of ΦAR should be controlled precisely for minimizing APP and improving the SPAD performance in high-speed photon counting applications.
KW - Active recharge circuit
KW - afterpulsing probability
KW - backside-illuminated (BSI) CMOS image sensor
KW - single-photon avalanche diode (SPAD)
KW - single-photon counting
UR - https://www.scopus.com/pages/publications/105011646450
U2 - 10.1109/ACCESS.2025.3591115
DO - 10.1109/ACCESS.2025.3591115
M3 - Article
AN - SCOPUS:105011646450
SN - 2169-3536
VL - 13
SP - 130517
EP - 130524
JO - IEEE Access
JF - IEEE Access
ER -