Waveguide SPAD Array Layout for NIR Detection With Low Timing Jitter
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Solution Overview
Problem
Current silicon-based single photon avalanche diodes (SPADs) for LiDAR systems face challenges in near-infrared detection due to high absorption depth and timing jitter, with open junction SPADs having poor time resolution and shallow junction SPADs having low photon detection efficiency.
Innovation Solution
A detector array with integrated waveguides and SPADs of varying widths, using a silicon-on-insulator substrate, where the SPADs are partitioned into independent segments with smaller dimensions to reduce timing jitter and enhance photon detection efficiency, and an end layer with a lower refractive index to reflect unabsorbed photons back into the waveguide.
Engineering Contradictions & Design Principles
Engineering Contradiction Analysis
1Reliability
If the SPAD junction width is increased to several 10 μm to detect single photons with high detection efficiency in the NIR, then the photon detection efficiency is improved, but the breakdown voltage increases to several 100V and the timing jitter increases due to uncertainty in carrier generation position (about 10 ps per 1 μm)
Solution Approach 1:
The patent divides the detector into multiple independent pixel elements, each with its own small SPAD junction. This segmentation allows each pixel to have low timing jitter while the array provides high photon detection efficiency through multiple detection opportunities. The segmentation principle resolves the contradiction by distributing the detection function across multiple small units rather than relying on a single large junction.
Solution Approach 2:
The patent transitions from a single large SPAD junction to a two-dimensional array of small SPADs. This dimensional change allows the system to achieve high photon detection efficiency through spatial distribution rather than increasing individual junction width, thereby maintaining low timing jitter while improving overall detection efficiency.
2Device complexity
If an open junction SPAD is used, then the device structure is simpler, but the timing resolution spreads due to drift component and diffusion tail from carriers generated in field-free regions
Solution Approach 1:
The patent implements a closed junction structure where the depletion region is fully extended into the substrate, creating a high electric field throughout the entire detection volume. This local quality change eliminates field-free regions, preventing carrier drift and diffusion tails, thereby achieving superior timing resolution. The closed junction design prioritizes timing precision over structural simplicity.
Solution Approach 2:
The patent changes the electrical field distribution parameter by implementing a closed junction with full substrate depletion. This parameter change transforms the electric field from having field-free regions (open junction) to being uniformly present throughout the detection volume (closed junction), eliminating the diffusion tail and improving timing resolution.
3Measurement precision
If a shallow junction SPAD is used to achieve better time resolution and reduced diffusion tail, then the timing resolution is improved, but the photon detection efficiency in the near infrared range is reduced due to limited silicon volume
Solution Approach 1:
The patent uses an array of multiple shallow junction SPADs instead of a single deep junction SPAD. Each shallow junction maintains excellent timing resolution, while the array configuration increases the total detection probability for NIR photons through spatial distribution and multiple detection opportunities, resolving the efficiency limitation of individual shallow junctions.
Solution Approach 2:
The patent compensates for the limited silicon volume of shallow junctions by extending the detection capability into the spatial dimension through a two-dimensional array. This dimensional transition allows the system to achieve high photon detection efficiency through increased pixel count rather than increasing individual pixel depth, thereby maintaining both shallow junction timing advantages and high NIR detection efficiency.
Applied Scientific Principles
This section explains which scientific principles are used to turn an abstract innovation direction into a practical engineering solution.
Function Achieved in This Case
The solution improves photon detection efficiency and time resolution by reducing dead time and increasing the probability of photon absorption, while maintaining low timing jitter and high spatial resolution in LiDAR systems.
Implementation Method 1
a detector array with integrated waveguides... using a silicon-on-insulator substrate... an end layer with a lower refractive index to reflect unabsorbed photons back into the waveguide
Implementation Method 2
single photon avalanche diode (SPAD)... adapted for use in the preferred wavelength ranges... detect single photons with high detection efficiency
Implementation Method 3
single photon avalanche diode (SPAD)... high breakdown voltages of several 100V... strongly reduced diffusion tail
Data Source
AI summary
A detector array (200) (200) according to the present teachings includes: a substrate (101) (101) adapted to function as a core layer of an optical waveguide (210) (210); a plurality of single photon avalanche photodiodes (SPAD (100)s (201)) disposed along a width of the substrate (101); a first cladding layer (202) (202) disposed over the plurality of SPADs (201) and along the width; and a second cladding layer (206) (206) disposed above the substrate and along the width.


