Large-area CMOS SPADs with very low dark counting rate

We designed and characterized Silicon Single-Photon Avalanche Diodes (SPADs) fabricated in a high-voltage 0.35 μm CMOS technology, achieving state-of-the-art low Dark Counting Rate (DCR), very large diameter, and extended Photon Detection Efficiency (PDE) in the Near Ultraviolet. So far, different groups fabricated CMOS SPADs in scaled technologies, but with many drawbacks in active area dimensions (just a few micrometers), excess bias (just few Volts), DCR (many hundreds of counts per second, cps, for small 10 μm devices) and PDE (just few tens % in the visible range). The novel CMOS SPAD structures with 50 μm, 100 μm, 200 μm and 500 μm diameters can be operated at room temperature and show DCR of 100 cps, 2 kcps, 20 kcps and 100 kcps, respectively, even when operated at 6 V excess bias. Thanks to the excellent performances, these large CMOS SPADs are exploitable in monolithic SPAD-based arrays with on-chip CMOS electronics, e.g. for time-resolved spectrometers with no need of microlenses (thanks to high fillfactor). Instead the smaller CMOS SPADs, e.g. the 10 μm devices with just 3 cps at room temperature and 6 V excess bias, are the viable candidates for dense 2D CMOS SPAD imagers and 3D Time-of-Flight ranging chips.

[1]  E. Charbon,et al.  A Single Photon Avalanche Diode Implemented in 130-nm CMOS Technology , 2007, IEEE Journal of Selected Topics in Quantum Electronics.

[2]  W. Brockherde,et al.  SPAD Smart Pixel for Time-of-Flight and Time-Correlated Single-Photon Counting Measurements , 2012, IEEE Photonics Journal.

[3]  Franco Zappa,et al.  Evolution and prospects for single-photon avalanche diodes and quenching circuits , 2004 .

[4]  B. Krauskopf,et al.  Proc of SPIE , 2003 .

[5]  N. Gisin,et al.  Low jitter up-conversion detectors for telecom wavelength GHz QKD , 2006 .

[6]  A. Lacaita,et al.  Avalanche photodiodes and quenching circuits for single-photon detection. , 1996, Applied optics.

[7]  D. G. Kocher,et al.  Three-Dimensional Imaging Laser Radars with Geiger-Mode Avalanche Photodiode Arrays , 2002 .

[8]  A. Tosi,et al.  Two-Dimensional SPAD Imaging Camera for Photon Counting , 2010, IEEE Photonics Journal.

[9]  D. Stoppa,et al.  Single-Photon Avalanche Diode CMOS Sensor for Time-Resolved Fluorescence Measurements , 2009, IEEE Sensors Journal.

[10]  Edoardo Charbon,et al.  Real-time fluorescence lifetime imaging system with a 32 x 32 0.13microm CMOS low dark-count single-photon avalanche diode array. , 2010, Optics express.

[11]  A. Lacaita,et al.  Trapping phenomena in avalanche photodiodes on nanosecond scale , 1991, IEEE Electron Device Letters.

[12]  R. Henderson,et al.  Edinburgh Research Explorer A Low Dark Count Single Photon Avalanche Diode Structure Compatible with Standard Nanometer Scale CMOS Technology , 2009 .

[13]  Alberto Tosi,et al.  Low-noise and large-area CMOS SPADs with timing response free from slow tails , 2012, 2012 Proceedings of the European Solid-State Device Research Conference (ESSDERC).

[14]  E. Charbon,et al.  A low-noise single-photon detector implemented in a 130 nm CMOS imaging process , 2009, ESSDERC 2009.

[15]  A. Tosi,et al.  Single-Photon Avalanche Diode Model for Circuit Simulations , 2007, IEEE Photonics Technology Letters.

[16]  F Panzeri,et al.  Custom single-photon avalanche diode with integrated front-end for parallel photon timing applications. , 2012, The Review of scientific instruments.

[17]  A. Lacaita,et al.  New silicon epitaxial avalanche diode for single-photon timing at room temperature , 1988 .

[18]  Edoardo Charbon,et al.  A single photon avalanche diode array fabricated in 0.35-μm CMOS and based on an event-driven readout for TCSPC experiments , 2006, SPIE Optics East.

[19]  Sergio Cova,et al.  Optical time-domain reflectometry with centimetre resolution at 10−15 W sensitivity , 1986 .

[20]  Franco Zappa,et al.  Variable-load quenching circuit for single-photon avalanche diodes. , 2008, Optics express.

[21]  C. Niclass,et al.  A miniature actively recharged single-photon detector free of afterpulsing effects with 6ns dead time in a 0.18µm CMOS technology , 2010, 2010 International Electron Devices Meeting.

[22]  P.D. Townsend,et al.  Experimental investigation of the performance limits for first telecommunications-window quantum cryptography systems , 1998, IEEE Photonics Technology Letters.

[23]  S. Cova,et al.  Progress in Silicon Single-Photon Avalanche Diodes , 2007, IEEE Journal of Selected Topics in Quantum Electronics.