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Contact Person :
Wendy Wang
Phone Number :
+86 27 50185150
Cooled LWIR Infrared Detector Integrated Into EO-IR Systems 640x512 15μm
| Place of Origin | Wuhan, Hubei Province, China |
|---|---|
| Brand Name | SensorMicro |
| Certification | ISO9001:2015; RoHS; Reach |
| Model Number | C615S LWIR |
| Minimum Order Quantity | 1 Piece |
| Price | Negotiable |
| Payment Terms | L/C,T/T |
Product Details
| Resolution | 640x512 | Pixel Pitch | 15μm |
|---|---|---|---|
| Stable Power Consumption | ＜8W | High Sensitivity | NETD≤25mK |
| Spectral Range | 3.7~4.8μm (MW); 7.7~9.5 (LW) | Size | 142x58.5x71mm |
| Highlight | Integrated LWIR Infrared Detector,640x512 Cooled LWIR Detector,Cooled LWIR Infrared Detector 15uM |
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Product Description
T2SL 640x512 / 15µm LWIR Cooled Infrared Detector with Integrated Dewar Cooler Assembly
Product Description
C615S LWIR integrated dewar cooler assembly is one of T2SL cooled infrared detectors developed by SensorMicro. It is a 640x512 / 15µm Type II Superlattice (T2SL), Integrated Detector Cooler Assembly (IDCA), designed for high performance 7.7~9.5μm Long Wave Infrared (LWIR) wavebands.
With 640x512 resolution and reduced pixel pitch to 15µm, the C615S LWIR integrated dewar cooler assembly provides clear image and superior performance. It features in most advanced technology, high quantum efficiency, high frame rate, high sensitivity, low noise, best non-uniformity etc.
As a LWIR detector, it presents high performance under the conditions of sand or dust climate and will not be affected by sunlight flicker or any high temperature flame.
Main Features
- Resolution: 640x512
- Pixel Pitch: 15µm
- High Sensitivity
- Good Imaging Effect
- Low Noise
- Stable Performance
- Excellent Non-uniformity
Product Specifications
| Model | C615S LWIR |
| Material | T2SL |
| Resolution | 640x512 |
| Pixel Pitch | 15um |
| Spectral Range | 7.7μm～9.5μm LW |
| Working Mode | Snapshot; ITR & Interlace Binning Integration Mode; Windows Mode; Anti-blooming |
| Charge Capacity | ITR: 12.22Me-/6.67Me- Interlace Binning: 24.44Me-/13.33Me- |
| Dynamic Range | ITR: ≥76dB Interlace Binning: ≥77dB |
| Output Channel | 4; Up to 22.5 Mpixel/s per Output |
| NETD | ≤30mK(F2 ITR) ≤25mK(F2 Interlace Binning) |
| Effective Pixel Rate | ≥99.5% |
| Response Non-uniformity | ≤8% |
| Cooler Type | RS058 |
| Steady Power Consumption | <8W |
| Max Power Consumption | <17W |
| Power Supply | 24V DC |
| Cooling Time | <5min30s |
| Weight | ≤600g |
| Dimension (mm) | 148x58.5x71 |
| Working Temperature | -45°C ~ +71°C |
Industrial Applications
The C615S LWIR cooled IR detector is widely used many areas such as Remote Monitoring System, Flight Vision Enhancement System, Multi-sensor Payload etc.
Standardized Service
Complete Documentation: Product manuals, setup guides, and selection references. Get started without guesswork.
Development & Testing Assistance: Sample Integrated Testing, performance evaluation, and parameter verification made easy.
Advanced Developer Toolkit: SDKs, APIs, algorithms, and debugging tools for deep integration.
Remote Technical Support: 24/7 support—quick response and timely resolution for critical issues.
Warranty: Original parts and strict process adherence to restore optimal performance.
FAQs
1. Advantages of Optical Gas Imaging
Time-saving & Efficient: support large-scale real-time detection, rapid leak location, no need for interrupting production.
Long Range Detection: away from dangerous and complex areas, non-contact non-destructive testing, without additional radiation source
Easy to Analyze: intuitive imaging, instant storage, convenient analysis
Multi-function Inspection: a variety of gases can be detected, with excellent remote temperature measurement function
2．Working Principle of Optical Gas Imaging
Optical gas imaging is a kind of infrared technology that could see invisible industrial gases.
After absorbing infrared radiation at specific wavelengths, infrared radiation difference will cause between the gas and the background.
The gas leak detection infrared detector with built-in narrowband filter only receives the infrared band near the gas infrared absorption peak, and can convert the gas into visible infrared images through the radiation difference between the gas and the background.
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