Faraday Mirror
A property of the Faraday mirror is that at any position in the fiber, regardless of the birefringence of the fiber, the polarization state of the forward transmission light and the polarization state of the reflected light always remain orthogonal. Therefore, Faraday mirror can be used to eliminate the polarization sensitivity of optical fiber systems and eliminate the power fluctuations caused by polarization in optical fiber interferometers and optical fiber laser systems.
Product Features：
- High Isolation
- Low Insertion Loss
- High Return Loss
- Low Polarization Sensitivity
- Optical Path Epoxy Free
Product Application：
- Optical Amplifier
- CATV Fiberoptic Links
- Fiberoptic Systems Test
- Fiberoptic LAN Systems
- Telecommunications
Product Parameters：
|
Parameter |
Unit |
Specification |
|
|
Center Wavelength |
nm |
1310, 1480, or 1550 |
|
|
Band Width |
Min |
nm |
±15 |
|
Typical Insertion Loss |
Max |
dB |
0.4 |
|
Maximum Insertion Loss |
Max |
dB |
0.6 |
|
Return Loss |
Min |
dB |
50 |
|
Faraday Rotation Angle (Single Pass) |
Deg |
45° |
|
|
Rotation Angle Tolerance over Wavelength and Temperature |
Deg |
0.5° |
|
|
Polarization Dependent Loss |
Max |
dB |
0.05 |
|
Polarization mode dispersion |
Max |
ps |
0.05 |
|
Power Handling |
mW |
300 |
|
|
Operating Temperature |
℃ |
-5~+70 |
|
|
Storage Temperature |
℃ |
-40~+85 |
|
|
Tensile Load |
N |
5 |
|
|
Package Dimension |
mm |
Φ4.5x25 or Φ5.5x30 |
|
Specifications may change without notice.
