A SiPM (silicon photomultiplier, also called a multipixel photon counter, MPPC) is an array of hundreds to tens of thousands of identical Geiger-Avalanche Photodiode (G-APD) cells, each approximately 1~100 μm in diameter, integrated in parallel on a monocrystalline silicon chip. Each cell is connected in series with a resistor of hundreds of kilohms to quench the large avalanche current promptly. All cells share a signal electrode and operate in Geiger mode, several volts above the cell breakdown voltage. Each silicon photomultiplier consists of many hundreds or thousands of APD cells, each comprising an APD in series with a high-value quenching resistor, connected in parallel as an area array. With reverse bias, generally tens of volts, a strong electric field forms in each APD depletion region. The source offers the simplified, explicitly imprecise explanation that an incoming photon undergoes Compton scattering with electron-hole pairs, releasing an electron or hole. High-energy carriers accelerate in the field and create many secondary carriers, producing an avalanche. The resulting increase in cell current increases the voltage drop across quenching resistor R and rapidly lowers the APD field, stopping the avalanche after a transient current pulse. Equal quenching resistances mean that cells theoretically produce equal pulses. Although APDs are analog devices, each cell behaves macroscopically as a logic element: output is “1” when a signal is present and “0” otherwise. Within the SiPM dynamic range, output current is proportional to the number of cells undergoing avalanches.
| Parameter | Value |
| Spectral response range λ | 320 to ~900 |
| Peak sensitivity wavelength λp [Depends on the die model] | 360~470( Depends on the die model ) |
| Temperature for stable signal output [Ta=25℃±10℃] | typical:±5 % |
| Photosensitivity Rv | min:2.1×106;typical:2.6×106;max:3.2×106 |
| Rise Time | typical:2 ns |
| Photoresponse pulse FWHM | typical:4 ns |
| Photon counting frequency fc | max:80 MHz |
| Dark count rate (at recommended bias) DCR | typical:~400 KHz |
| Noise Equivalent Power NEP [Complete darkness] | typical:3 fw/Hz1/2 |
| Number of resolved photons for pulsed light (average) PNR | min:0.1 units;typical:20 units;max:47 units |
| Saturating incident optical flux Pin | typical:~100 nW |
Widely used in high-energy physics and nuclear medicine (PET), biomedicine, fluorescence spectroscopy, lidar and laser ranging, and widely regarded as a future direction for extremely weak-light detectors. High-energy physics: photodetectors must operate in extremely strong magnetic fields, with very demanding requirements for PDE (detection efficiency) and dark noise. Nuclear medicine (PET): PET is the only new imaging technology capable of showing biomolecular metabolism, receptor activity and neurotransmitter activity in living organisms. It is widely used for diagnosis and differential diagnosis of diseases, assessment of disease status and treatment response, organ-function research and new-drug development. Magnetic resonance imaging is a biological magnetic-spin imaging technology. It directly produces transverse, sagittal, coronal and various oblique tomographic images, without the artifacts found in CT examinations, without ionizing radiation and without adverse effects on the body. MR is highly effective for detecting common cranial conditions such as intracerebral and extracerebral hematomas, brain tumors, intracranial aneurysms, arteriovenous malformations, cerebral ischemia, intraspinal tumors, syringomyelia and hydromyelia. It is also effective for diagnosing conditions such as posterior lumbar-disc herniation and primary liver cancer. Combining PET and MR imaging would greatly benefit the diagnosis of tumors, breast cancer and other diseases. However, photomultiplier tubes (PMT), the photodetectors used in PET, cannot operate in the strong magnetic field of MR, hindering this combination. Replacing PMT with silicon photomultipliers resolves this problem. PET/CT. Precision analysis: this field addresses detection, analysis and metrology of extremely low photon fluxes, even at the single-photon level, in biosensing equipment such as fluorescence detectors and flow cytometers. SiPM offers high detection efficiency in the visible range, a fast response and lower prices than electron-tube detectors such as PMT, making it a commonly used photodetector for precision analysis. Laser detection and measurement: LiDAR (Light Detection And Ranging) is a laser-scanning technology integrating laser ranging, computing and inertial measurement units. It is an important means of acquiring three-dimensional spatial information in real time [5]. LiDAR is mainly based on TOF (Time of Flight), imposing stringent requirements on detector timing performance and detection efficiency. SiPM is among the few detectors able to meet these requirements. SiPM can provide the best signal-to-noise performance for long-distance ranging in bright sunlight. Other advantages include lower supply bias and lower sensitivity to temperature changes, making it an ideal upgrade for systems using conventional avalanche photodiodes (APD). High-volume CMOS manufacturing enables the lowest detector costs and LiDAR solutions for broad markets. Laser ranging; lidar; X-ray irradiation security screening/container-scanning security screening; X-ray irradiation security screening; container-scanning security screening; lidar for automotive driver assistance. Laser distance measurement has extended across automotive, consumer and industrial applications. In vehicles, LiDAR can improve safety and advanced driver-assistance systems (ADAS), complementing other sensing modalities and providing redundancy for functions such as lane keeping and traffic-jam assistance. LiDAR is commonly used in fully autonomous applications such as robotic transport for safe, real-time navigation. SiPM achieves an industry-leading photon detection efficiency (PDE) of 18.5% at 905 nanometres (nm) (1). Its high internal gain enables single-photon sensitivity. Combined with high PDE, this allows detection of the weakest return signals and longer detection distances even for low-reflectivity targets.
1. High gain. 2. High sensitivity. 3. Low bias voltage. 4. Insensitive to magnetic fields. 5. Compact structure.
Dongguan Zhongke Atom Precision Manufacturing Technology Co., Ltd. is a high-tech enterprise focusing on photoelectric detection and laser sensing technologies. It is dedicated to the R&D and production of optical sensors such as super second-generation, third-generation, and ultrafast image intensifiers, photomultiplier tubes, electron/ion detection devices, as well as digital cameras like intensified cameras and low-light cameras. It also provides laser sensors including laser wind radar, ceilometer, TOF lidar, and instruments such as time-resolved Raman spectrometers and time-gated imagers. Products are widely used in low-light night vision, laser 3D surveying, industrial inspection, and scientific research. The company is located in Songshan Lake, Dongguan, with comprehensive OEM and customized solution capabilities.