A Lownoise Cmos Spad Pixel With 121 Ps Sptr And 3 Ns Dead Time
- doi: 10.1109/JSTQE.2021.3088216
-
title: A Low-Noise CMOS SPAD Pixel With 12.1 Ps SPTR
and 3 Ns Dead Time
- publisher: IEEE
- isbn:
- issn: 1558-4542
- rank: 791
-
access_type: CCBY - IEEE is not the copyright holder of
this material. Please follow the instructions via
https://creativecommons.org/licenses/by/4.0/ to obtain full-text
articles and stipulations in the API documentation.
- content_type: Journals
-
abstract: Single-photon avalanche diodes (SPADs) have
become the sensor of choice in many applications whenever high
sensitivity, low noise, and sharp timing performance are required,
simultaneously. Recently, SPADs designed in CMOS technology, have
yielded moderately good performance in these parameters, but never
equaling their counterparts fabricated in highly customized,
non-standard technologies. The arguments in favor of CMOS-compatible
SPADs were miniaturization, cost and scalability. In this paper, we
present the first CMOS SPAD with performance comparable or better than
that of the best custom SPADs, to date. The SPAD-based design, fully
integrated in 180 nm CMOS technology, achieves a peak photon detection
probability (PDP) of 55% at 480 nm with a very broad spectrum spanning
from near ultraviolet (NUV) to near infrared (NIR) and a normalized dark
count rate (DCR) of 0.2 cps/$\mu$m$^2$, both at 6 V of excess bias.
Thanks to a dedicated CMOS pixel circuit front-end, an afterpulsing
probability of about 0.1% at a dead time of $\sim$3 ns were achieved. We
designed three SPADs with a diameter of 25, 50, and 100 $\mu$m to study
the impact of size on the timing jitter and to create a scaling law for
SPADs. For these SPADs, a single-photon time resolution (SPTR) of 12.1
ps, 16 ps, and 27 ps (FWHM) was achieved at 6 V of excess bias,
respectively. The SPADs operate in a wide range of temperatures, from
−65 $^{\circ }$C to 40 $^{\circ }$C, reaching a normalized DCR of 1.6
mcps/$\mu$m$^2$ at 6 V of excess bias for the 25 $\mu$m at −65 $^{\circ
}$C. The proposed SPADs are ideal for a wide range of applications,
including (quantum) LiDAR, super-resolution microscopy, quantum random
number generators, quantum key distribution, fluorescence lifetime
imaging, time-resolved Raman spectroscopy, to name a few. All these
applications can take advantage of the vastly improved performance of
our detectors, while enjoying the opportunities of megapixel resolutions
promised by the economy of scale that is offered by CMOS technologies.
- article_number: 9451600
-
pdf_url:
https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=9451600
-
html_url:
https://ieeexplore.ieee.org/document/9451600/
-
abstract_url:
https://ieeexplore.ieee.org/document/9451600/
-
publication_title: IEEE Journal of Selected Topics in
Quantum Electronics
- conference_location:
- conference_dates:
- publication_number: 2944
- is_number: 9497052
- publication_year: 2022
- publication_date: March-April 2022
- start_page: 1
- end_page: 9
- citing_paper_count: 42
- citing_patent_count: 0
- download_count: 5164
- insert_date: 20210610
-
index_terms:
-
ieee_terms:
- Single-photon avalanche diodes
- Temperature measurement
- Voltage measurement
- Sensitivity
- CMOS technology
- Transistors
- Delays
-
author_terms:
- Active reset
- cascode
- jitter
- low noise
- low power
- photon detection probability (PDP)
- pixel
- quantum key distribution (QKD)
- single-photon avalanche diode (SPAD)
- timing
-
dynamic_index_terms:
- Dead Time
- Single-photon Avalanche Diode
- Single Photon Avalanche Diode
- Single-photon Avalanche Diode Pixel
- High Performance
- Economies Of Scale
- Low Noise
- Count Rate
- near-UV
- Near-ultraviolet
- CMOS Technology
- Fluorescence Lifetime Imaging Microscopy
- FLIM
- Fluorescence Lifetime Imaging
- Noise Performance
- Quantum Key Distribution
- Timing Jitter
- Dark Count Rate
- Power Consumption
- Pulse Width
- Pulsewidth Modulation
- Pulsewidth
- Pulse Width Modulation
- Oscilloscope
- Photon Flux
- Photon Flux Density
- Large Array
- Second Harmonic Generation
- Scalable Architecture
- TCAD Simulation
- Inter-arrival Time
- Low Light Levels
-
authors:
-
Author Name: Francesco Gramuglia
Affiliation: Advanced Quantum Architecture
Laboratory (AQUA), École Polytechnique Fédérale de Lausanne (EPFL),
Neuchâtel, Switzerland
Author URL:
https://ieeexplore.ieee.org/author/37086064963
ID: 37086064963
Order: 1
Author Affiliations:
-
Advanced Quantum Architecture Laboratory (AQUA), École
Polytechnique Fédérale de Lausanne (EPFL), Neuchâtel,
Switzerland
-
Author Name: Ming-Lo Wu
Affiliation: Advanced Quantum Architecture
Laboratory (AQUA), École Polytechnique Fédérale de Lausanne (EPFL),
Neuchâtel, Switzerland
Author URL:
https://ieeexplore.ieee.org/author/37089300056
ID: 37089300056
Order: 2
Author Affiliations:
-
Advanced Quantum Architecture Laboratory (AQUA), École
Polytechnique Fédérale de Lausanne (EPFL), Neuchâtel,
Switzerland
-
Author Name: Claudio Bruschini
Affiliation: Advanced Quantum Architecture
Laboratory (AQUA), École Polytechnique Fédérale de Lausanne (EPFL),
Neuchâtel, Switzerland
Author URL:
https://ieeexplore.ieee.org/author/37274823200
ID: 37274823200
Order: 3
Author Affiliations:
-
Advanced Quantum Architecture Laboratory (AQUA), École
Polytechnique Fédérale de Lausanne (EPFL), Neuchâtel,
Switzerland
-
Author Name: Myung-Jae Lee
Affiliation: Post-Silicon Semiconductor Institute,
Korea Institute of Science and Technology (KIST), Seoul, South
Korea
Author URL:
https://ieeexplore.ieee.org/author/37598674000
ID: 37598674000
Order: 4
Author Affiliations:
-
Post-Silicon Semiconductor Institute, Korea Institute of Science
and Technology (KIST), Seoul, South Korea
-
Author Name: Edoardo Charbon
Affiliation: Advanced Quantum Architecture
Laboratory (AQUA), École Polytechnique Fédérale de Lausanne (EPFL),
Neuchâtel, Switzerland
Author URL:
https://ieeexplore.ieee.org/author/37271353200
ID: 37271353200
Order: 5
Author Affiliations:
-
Advanced Quantum Architecture Laboratory (AQUA), École
Polytechnique Fédérale de Lausanne (EPFL), Neuchâtel,
Switzerland
Image Sensor
- sensor_type: CMOS
- resolution: not specified in the text
- dynamic_range: not specified in the text
- pixel_size: 25 µm, 50 µm, and 100 µm
-
dark_current: 0.2 cps/µm² at 6 V excess bias; 1.6
mcps/µm² at -65 °C for 25 µm SPAD at 6 V excess bias; up to 4 mcps/µm²
at 8 V excess bias at -65 °C
Optical Data
- focal_length: not specified
- aperture: not specified
- field_of_view: not specified
- distortion: not specified
Performance Metrics
- frame_rate: up to 300 Mcps
- signal_to_noise_ratio: not specified in the text
-
sensitivity: peak photon detection probability of 55%
at 480 nm
- power_consumption: not specified in the text
-
noise: normalized dark count rate (DCR) of 0.2 cps/µm²
at room temperature
Applications & Benefits
-
cell_imaging: the SPADs are suitable for
super-resolution microscopy, fluorescence lifetime imaging, and
time-resolved Raman spectroscopy
-
benefits: high sensitivity, low noise, and sharp timing
performance suitable for quantum LiDAR, quantum key distribution, and
other applications
Supporting Organizations
-
supported_by: Swiss National Science Foundation under
Grants 200 021-169 465 and Sinergia CRSII5-177 165.
Manuscript Details
- publication_date: March-April 2022
Relevancy Score
- score: 8
-
missing_fields:
- resolution
- dynamic_range
- focal_length
- aperture
- field_of_view
- distortion
Processed JSON Filename
request_2881f3db-d1f6-49c7-b265-164191908e26-a_lownoise_cmos_spad_pixel_with_121_ps_sptr_and_3_ns_dead_time.json