PET Detection Module
Modular PET Module for Efficient Economical Scanner Construction,Comprehensive Customization for Unique Needs.
Save to Favorites
Overview
Specifications
| Parameter | Value |
|---|---|
| Scintillator | BGO, LYSO, GAGG Arrays, Fully Customizable Pixel/Array Size and Reflector Type |
| Detector | SiPM, Fully Customizable Pixel Size, Pitch and Array Dimensions |
| Light Guide | Fully Customizable |
| Readout Electronics | CAPNET + Integrated TDC/ADC Board |
| Performance | Comparable to ASIC Detectors |
| Power Consumption [Per Module] | Approximately 1W/Module |
| Energy Resolution (LYSO) | ~9% |
| Coincidence Time Resolution (LYSO) | ~310ps |
Datasheet
Please provide your email to download the datasheet.
Invalid email format. Please try again.
Supplier Information
Related Products
-
40G High-Speed Indium Gallium Arsenide (InGaAs) Photodetector HSPD4040
Optical Detectors
Fiberwdm
Storage Temperature Range TSTG [Typical Values and Absolute Maximum Ratings]: typical:-45~+85; Rated: -55~+85 Operating Case-Temperature Range TC [Typical Values and Absolute Maximum Ratings]: typical:25; Rated: -40~+85 Bias Voltage VR [Typical Values and Absolute Maximum Ratings]: typical:5; Rated: 5~6
HSPD4040 is a high-speed detector module for digital/analog applications. An InGaAs PIN photodiode responds over1250–1650nm with matching electronics. Maximum bandwidth is40GHz, supply+5V, input standard single-mode9/125μm fiber, and RF output a2.92mm connector matched to50ohms. A sealed housing weighs under20g. The description states ROHS2.0 compliance with restrictions on hazardous substances in electrical/electronic equipment. After nearly two years of R&D,广州瑞东 developed two fully domestic high-speed PD products described as exceeding18GHz and40GHz bandwidth. The18GHz version has rise time<20ps and the40GHz PD<8.5ps. Responsivity is described as matching or exceeding comparable Finisar/Thorlabs imports,with well-controlled tail ringing. Without a TIA,the detectors provide very low noise for high-speed communications and femtosecond-laser testing at high cost effectiveness. The company's independently developed linear supply meets research needs for these detectors.
-
Biased Detector Series PD1500/PD2100
Optical Detectors
Fiberwdm
Wavelength Range: 900nm-1700nm 3dB Cutoff Bandwidth: 5GHz Saturation Optical Power: 5mW
This detector series is a direct replacement for Thorlabs battery-powered products and is described as matching or exceeding equivalent Thorlabs products in all performance aspects. In addition to standard specifications, customization can adjust parameters such as supply voltage and bandwidth to customer requirements. Designed specifically for laser measurement systems, the series has an internal battery and no gain amplification, offering a cost-effective detector for high-power laser laboratories.
-
Biased Detector Series PD1500/PD2100
Optical Detectors
Fiberwdm
Wavelength Range: 320nm-1000nm 3dB Cutoff Bandwidth: 1GHz Saturation Optical Power: 5mW
This detector series is a direct replacement for Thorlabs battery-powered products and is described as matching or exceeding equivalent Thorlabs products in all performance aspects. In addition to standard specifications, customization can adjust parameters such as supply voltage and bandwidth to customer requirements. Designed specifically for laser measurement systems, the series has an internal battery and no gain amplification, offering a cost-effective detector for high-power laser laboratories.
-
High-Speed Detector HSPD4018
Optical Detectors
Fiberwdm
Wavelength Range: 1000nm - 1700nm 3dB Cutoff Bandwidth: 18GHz Conversion Gain: 35V/W
After nearly two years of R&D,广州瑞东 developed two fully domestic high-speed PD products described as exceeding18GHz and40GHz bandwidth. The18GHz version has rise time<20ps and the40GHz PD<8.5ps. Responsivity is described as matching or exceeding comparable Finisar/Thorlabs imports,with well-controlled tail ringing. Without a TIA,the detectors provide very low noise for high-speed communications and femtosecond-laser testing at high cost effectiveness. The company's independently developed linear supply meets research needs for these detectors.
-
PDA1000-2 Dual-Channel 10KHz Single-Element Detector
Optical Detectors
Fiberwdm
Wavelength Range [Model PDA1000-2 in the Technical Table]: 900-1700nm dB Bandwidth [Model PDA1000-2 in the Technical Table]: 10kHz Conversion Gain [Technical Table Model PDA1000-2; High-Impedance Output Load; Gain Halved from Nominal with 50Ω Load]: 2.5×10⁴V/A
This detector series operates much like single-element detectors from Thorlabs and Newport and has identical power interfaces. It can directly replace equivalent products when Monitor output is unnecessary and bandwidth matches, with performance described as matching or exceeding comparable Thorlabs/Newport detectors. Beyond standard versions, customization adjusts supply voltage, gain, bandwidth and other parameters to customer requirements.
Related Articles
In photonics and laser technology, devices that manipulate optical signals via the electro-optic effect form the backbone of precision optical systems. Electro-optic phase modulators and electro-optic deflectors are two prominent examples of this device category. As a critical hardware solution for high-speed, high-accuracy laser beam direction control, electro-optic deflectors are widely deployed across industrial and research settings. Below is a detailed overview of their core structure, key performance drivers, and primary use cases.
GYOPTICS 30 W collimated isolator is a highly‑reliable passive optical component optimized for 1064 nm high‑power laser systems. Characterized by low insertion loss and superior backward‑light suppression capability, it effectively blocks reflected light traveling back toward the laser resonator, eliminating back‑reflection‑induced instability and protecting fiber or solid‑state laser sources during long‑term operation.
For 1D optical detection scenarios such as spectrum acquisition, dimensional measurement and optical scanning, area array CMOS/CCD suffer redundant pixels, high cost and slow row readout speed.
Laser pump sources are the core energy input component of solid-state lasers and laser amplifiers, and their performance directly determines the output power, beam quality and service life of the entire laser system. In scenarios such as industrial processing, scientific research experiments and high-end equipment, improper pump source selection will not only result in substandard system performance, but also bring a series of problems such as rapid device degradation and high operation and maintenance costs. This article sorts out the core selection logic and key pitfalls of pump source procurement, and provides selection references based on mature, mass-produced high-reliability products to help purchasers efficiently screen suitable products.
Loading...
Name
Phone
Organization
Use Case
Database Platform