Description
Fiber Raman amplifier uses the Raman effect in quartz fiber to provide gain to optical signals, and achieves high gain and low noise amplification of optical signals in the C or L band, which can effectively compensate for the attenuation of optical signals in long-distance optical fiber transmission. It can be used in long-distance optical transmission systems, distributed optical fiber sensing, and intensive wavelength division multiplexing optical transmission systems.
Distributed Fiber Raman Amplifier
Specifications
| Amplifier Type: | Raman Amplifier |
|---|---|
| Wavelength Range: | 1528 – 1650 nm |
| Min Input Power: | Not Specified |
| Max Output Power: | Not Specified |
| Nominal Gain: | 14 dB |
| Output Fiber Type: | SMF-28 |
| Signal Wavelength: | 1528-1565 nm, 1570-1650 nm |
| Raman Gain: | 10/20 dB |
| Gain Flatness: | 2 dB |
| Pump Wavelength: | 1425-1457 nm, 1470-155 0nm |
| Pump Power: | 300/500/1000/1400 mW |
| Pump Light Polarization: | 5% (Typ.), 10% (Max.) |
| Polarization Dependent Gain: | 0.2 dB |
| Polarization Mode Dispersion: | 0.5 dB |
| Input/Output Isolation: | 35 dB |
| Optical Connector: | FC/APC or Fiber Collimator |
| Control Mode: | Automatic Pump Power Control (APPC) |
Got questions about specs? Use the inquiry form to ask.
Features
- Low noise
- High gain
- Wide wavelength range
Applications
- Optical fiber distributed sensing
- Fiber lasers
- Long-distance optical
Frequently Asked Questions
What is a Distributed Fiber Raman Amplifier?
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