30 products
10Gb/s SFP Transceiver - DWDM, 40km Reach
1 x ¥116,880.50 = ¥116,880.50CWDM DFB Optical Laser Source
2 x ¥324,010.49 = ¥648,020.99Nx1 Multimode Power Combiner for Fiber Lasers
2 x ¥0.00 = ¥0.00Optical Fiber Fusion Splicer - Light Weight
1 x ¥443,702.04 = ¥443,702.04Direct Buried Optical Fiber Cable - 24 to 312 Fibers, G652.D
1 x ¥0.00 = ¥0.001550nm DFB Laser Diode - High Power Butterfly Package
1 x ¥332,887.49 = ¥332,887.49Dispersion Compensation Fiber - C Band
2 x ¥0.00 = ¥0.0010Gb/s Surface-Mount PIN/TIA Detector
3 x ¥0.00 = ¥0.00Optical Fiber Splicing Protector - Heat Shrinkable
1 x ¥5,903.20 = ¥5,903.20Semiconductor Optical Amplifier (SOA) - High Power
1 x ¥0.00 = ¥0.00Polarization Maintaining (PM) Optical Coupler - 2 micron meter
1 x ¥295,752.04 = ¥295,752.04Optical Fiber Identifier
1 x ¥131,675.50 = ¥131,675.50Visual Fiber Fault Finder - 10mW
1 x ¥11,688.05 = ¥11,688.05Optical Fiber Fusion Splicer
1 x ¥738,270.48 = ¥738,270.48EPON OLT Optical Transceiver - 1.25Gbps SFF Module
1 x ¥43,645.25 = ¥43,645.25Mini Broadband ASE Light Source - 1060nm
1 x ¥1,109,624.98 = ¥1,109,624.98Variable Optical Attenuators - Adapter Type
1 x ¥2,957.52 = ¥2,957.52Gain Flattening Filter for Optical Amplifiers
1 x ¥51,782.50 = ¥51,782.5040-Channel 100GHz Athermal AWG Module
1 x ¥190,855.50 = ¥190,855.50Optical Source DFB 1310nm
1 x ¥303,297.49 = ¥303,297.49Uncooled 1310nm SLED Diode - Coaxial Pigtailed
1 x ¥44,237.05 = ¥44,237.0510Gb/s Pluggable SFP+ Transceiver - 1310nm 10km
1 x ¥17,606.05 = ¥17,606.05DWDM DFB Optical Laser Source
1 x ¥547,414.99 = ¥547,414.99Handheld Variable Optical Attenuator - 850 or 1310nm MMF
1 x ¥133,007.05 = ¥133,007.05Super Wide Spectrum Light Source - SLED
1 x ¥0.00 = ¥0.00- ¥5,169,208.67
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Optical Fiber Mirror - Faraday Rotator [FRM]
¥10,785.55¥9,764.70-
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Displaying 1 to 1 (of 1 reviews)Result Pages: 1Date Added: Sunday 12 February, 2012 by Technology ExplainedFaraday rotator is a device that exploits the magnetic optical effect in certain crystals. When magnetic field is applied to the crystal, it changes the refractive index of the crystal. When a linearly polarized light passes through the crystal at the same direction of the magnetic field lines, and we know that the linearly polarized light can be treated as the superposition of two circularly polarized components (with opposite circular direct..Rating: [5 of 5 Stars!]Displaying 1 to 1 (of 1 reviews)Result Pages: 1
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