*Click on the images for larger view*
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Optical beams traveling in a single mode fiber experience random birefringence, which could make it difficult or impossible for fiberoptic Michelson interferometer to function properly. Faraday rotator mirrors take the output beam from a single mode fiber and rotate the polarization by 90 degrees before sending it back through the same fiber. By doing so, a Faraday mirror functions as a phase conjugate mirror and cancels out any birefringent effects the beam experienced along the forward path.
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Princetel’s FRM series Faraday rotator mirrors offer strong suppression against secondary reflections (-55 dB), a feature critical to most interferometer applications.
SPECIFICATIONS
CREATE YOUR PART NUMBER
PARAMETERS | VALUES |
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![]() | 1310 or 1550 nm |
![]() | <1 dB (typical: 0.5 dB) |
![]() | <+/-2 deg. (typical: <+/-1 deg.) |
![]() | >55 dB (non reflective surfaces) |
![]() | 10 N (900 um jacket) |
![]() | 23 dBm |
![]() | -40 to 65 C/FRM, -20 to 65 C/FRM4 |
![]() | -60 to 85 C/FRM, -40 to 75 C/FRM4 |
![]() | 95% RH non condensing |
![]() | Stainless steel |
![]() | Corning SMF28 with 900 um buffer |
![]() | FC, SC, ST, SMA, or LC (& APC counterparts) |
![]() | 6×9 mm (diaxL)/FRM, 4×20 mm (diaxL)/FRM4 |
![]() | 4 g/FRM, 2 g/FRM4 |
FRM- wavelength code– fiber code– connector code
FRM4- wavelength code– fiber code– connector code
*click a link to see codes*
DOCUMENTS DOWNLOAD | |
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