19–22 Nov 2024
Harbour Centre, Vancouver (BC), Canada
US/Pacific timezone

Development of Active-Quenching SPAD Array Based on the Tri-State Gates of FPGA and Packaging of Bare Chip Stacking

20 Nov 2024, 11:59
18m
Room: 1400-1430 (Harbour Centre, Vancouver (BC), Canada)

Room: 1400-1430

Harbour Centre, Vancouver (BC), Canada

515 West Hastings Street, Vancouver, BC V6B 5K3
Oral/Presentation Digital Photonsensors Digital Photosensors (2) (Chair: Guido Haefeli, Kurtis Raymond)

Speaker

Dr liangliang liu (Novel Device Laboratory (NDL), School of Physics and Astronomy, Beijing Normal University)

Description

Abstract: We present the development of a fully reconfigurable, active-quenching, single photon avalanche diode (SPAD) array. It is fabricated by integrating a bare chip of Field-Programmable Gate Array (FPGA) with a bare die of 4×4 SPAD array with three-dimensional stacked package. The active quenching is realized through the Tri-State Gates and Look-Up Tables (LUTs) of the FPGA. This architecture ensures complete separation of the quenching mechanism from any kind of avalanche photodiode (APD) array (e.g., non-silicon material based APDs), facilitating independent and tailored design of the SPAD array. Compared to a system-on–chip (SOC) based SPAD array, our approach provides a significantly quicker and more flexible deployment, lower startup costs, and is well-suited for developmental stages and lower volume applications.In this study, the SPAD array utilizes an N-on-P design, the pitch of pixels was 60 µm. By setting the dead time of 200 ns and over voltage of 3.2V, it demonstrated afterpulsing rates range from 1.19% to 2.04%, dark count rates range from 93 kcps/pixel to 108 kcps/pixel, crosstalk of 11.8% from the nearest-neighbor pixel and 4.3% from next-nearest-neighbor pixel. It also demonstrated a linear response up to 20MHz. We designed a Time-to-Digital Converter (TDC) for each pixel by employing the same FPGA. These TDCs boast a least significant bit (LSB) ranging from 25.8 ps to 26.3 ps and achieved a time resolution of approximately 1.17 ns for individual pixel under a 532-nm pulse light source. This kind of SPAD array has potential to be applied in fluorescence analysis and transient imaging with great simplicity and flexibility.

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Author

Dr liangliang liu (Novel Device Laboratory (NDL), School of Physics and Astronomy, Beijing Normal University)

Co-authors

Dejun Han (Novel Device Laboratory (NDL), School of Physics and Astronomy, Beijing Normal University) Jian Liu (Novel Device Laboratory (NDL), School of Physics and Astronomy, Beijing Normal University) Kun Liang ((Novel Device Laboratory (NDL), School of Physics and Astronomy, Beijing Normal University)) Ru Yang ((Novel Device Laboratory (NDL), School of Physics and Astronomy, Beijing Normal University)) Mr Wenxing Lv (Novel Device Laboratory (NDL), School of Physics and Astronomy, Beijing Normal University) Dr Xingan Zhang (Novel Device Laboratory (NDL), School of Physics and Astronomy, Beijing Normal University) Mr jiawen chen (Novel Device Laboratory (NDL), School of Physics and Astronomy, Beijing Normal University)

Presentation materials