InGaAs single photon avalanche diodes (SPADs) 

InGaAs single photon avalanche diodes (SPADs) 

It is a solid-state photodetector similar to photodiodes and avalanche photodiodes (APDs), while also being very much linked with basic diode behaviors.

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InGaAs single photon avalanche diodes (SPADs) 
InGaAs single photon avalanche diodes (SPADs) 

For example

InGaAs Geiger mode avalanche photodiode (Built-in TEC cooling type)  

parametersymbolunitsconditionsmintypmax
Reverse  breakdown voltageBRV22℃±3℃ ,ID =10μA608090
ResponsivityReA/W22℃±3℃,λ =1550nm ,M =10.80.85
Dark currentIDnA22℃±3℃,M =100.10.3
CapacitanceCpF22℃±3℃ ,M =10,f=1MHz0.25
TemperatureηV/K-40℃ ~80℃,ID =10μA0.15

InGaAs Single-Photon Avalanche Diodes (SPADs)  

Geiger mode parameters

parametersunitTest conditionsmintypicalmax
Single Photon Detection Efficiency (PDE) %-45℃, λ =1550nm,0.1ph/pulsePoisson   distribution single photon source 20
 Dack count rate (DCR) kHz-45℃, 1ns gate   width,2MHz Gated repetition   frequency,1MHz Optical repetition frequency,PDE=20% 20*
After pulse probability (APP)-45℃, 1ns gate width,2MHz Gated repetition frequency,1MHz Optical repetition frequency,PDE=20% 1× 10-3
Time jitter (Tj)ps-45℃, 1ns gate width ,2MHz Gated repetition frequency,PDE=20%100

Back-incidence InGaAs Single-Photon Avalanche Diode Array Chip Series  

Spectral Range 950~1650nm; Pixel Num. 1×16; Active Diameter 50μm*16; Chip Dimensions 450μm×1050μm

Spectral Range 950~1650nm; Pixel Num. 4×4; Active Diameter 50μm*16; Chip Dimensions 800μm×800μm

Spectral Range 950~1650nm; Pixel Num.2×2; Active Diameter 50μm*4; Chip Dimensions 400μm×400μm

DC Characteristics Specifications *

ParameterSymbolTest ConditionMin.Typ.Max.Unit
Active DiameterΦ+454850μm
Spectral RangeΔλ9501650nm
Breakdown VoltageVBRIR =10μA, PIN =0507090V
DC Dark CurrentIDVR =VBR-2V, PIN =0110nA
1550nm-ResponsivityR1550VR =VBR-2V, PIN =10μW (1550nm)8.08.5A/W
CapacitanceCVR =VBR-2V, f=1MHz0.20.5pF
Vbr temperature coefficientηIR =10μA, PIN =0, -40~25℃0.100.15V/℃

* All tests are taken at room temperature if not indicated.

+ This is the backside micro-lens dimension.

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Similar products that are in top demand today are other photodetectors that offer competing or more advanced features, often in different spectral ranges or with different operating principles. The market is driven by a need for higher efficiency, lower noise, and different form factors.


1. Silicon Photomultipliers (SiPMs)

These are arrays of silicon SPADs, but are often used as single, integrated devices. They are a top-demand product for their ability to detect a wide range of light levels, from single photons to bright flashes. SiPMs are popular in LiDAR, medical imaging (PET), and high-energy physics.


2. Superconducting Nanowire Single-Photon Detectors (SNSPDs)

SNSPDs are the highest-performance single-photon detectors available. They offer near-perfect quantum efficiency, extremely low dark counts, and picosecond timing jitter. While they require cryogenic cooling, their unparalleled performance makes them a top choice for cutting-edge quantum communication and scientific research.


3. Silicon Avalanche Photodiodes (APDs)

An APD is a standard photodetector with internal gain. When operated in “Geiger mode,” an APD functions as a SPAD. Silicon APDs are the most common type of single-photon detector for the visible and near-infrared (NIR) spectrum, widely used in long-range LiDAR and range-finding due to their low cost and high reliability.


4. Photomultiplier Tubes (PMTs)

PMTs are classic vacuum tube-based detectors. They are still in top demand for low-light applications where a large active area is required, such as in high-energy physics, scintillation counting, and astronomy. They offer high gain and very fast response times.


5. Quantum Dot (QD) Photodetectors

Quantum dot technology is an emerging and highly promising field. Quantum dot photodetectors offer a tunable spectral response that can be tailored for specific applications in the visible and infrared ranges. Their potential for low-cost, high-performance manufacturing makes them highly sought after in research and development.


6. InGaAs Avalanche Photodiodes (APDs)

While InGaAs SPADs are used for single-photon detection, InGaAs APDs are the workhorse for high-speed, high-sensitivity detection in the SWIR range for applications that don’t require single-photon sensitivity. They are in high demand in the fiber-optic telecommunications industry for long-distance data transmission.


7. HgCdTe (MCT) Photodiodes

Mercury Cadmium Telluride is a versatile semiconductor material whose bandgap can be tuned to operate in the SWIR, MWIR, and LWIR (long-wave infrared). Cooled HgCdTe photodiodes offer high performance and are a top choice for scientific cameras and high-end thermal imaging.


8. Silicon PIN Photodiodes

A PIN photodiode is the most common and simple type of semiconductor detector. It is highly valued for its linearity, low cost, and fast response. It’s the workhorse for visible light sensing and power measurement, and while it lacks internal gain, it is a crucial component in countless optical systems.


9. Pockels Cells

While not a detector, a Pockels cell is an electro-optic modulator that is often paired with a photodetector for high-speed, precision light control. It is in demand for applications that require fast pulsing or switching of a laser beam, such as in Q-switched lasers or laser communication.


10. Ge-on-Si SPADs

Germanium on Silicon (Ge-on-Si) SPADs are an emerging technology. They combine the mature silicon manufacturing platform with the SWIR-sensitivity of germanium, creating a detector that is more cost-effective to produce than InGaAs SPADs. They are in high demand for mass-market applications like LiDAR for autonomous vehicles.

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