30 products
10Gb/s SFP Transceiver - DWDM, 40km Reach
1 x A$1,215.41 = A$1,215.41CWDM DFB Optical Laser Source
2 x A$3,369.31 = A$6,738.63Nx1 Multimode Power Combiner for Fiber Lasers
2 x A$0.00 = A$0.00Optical Fiber Fusion Splicer - Light Weight
1 x A$4,613.96 = A$4,613.96Direct Buried Optical Fiber Cable - 24 to 312 Fibers, G652.D
1 x A$0.00 = A$0.001550nm DFB Laser Diode - High Power Butterfly Package
1 x A$3,461.62 = A$3,461.62Dispersion Compensation Fiber - C Band
2 x A$0.00 = A$0.0010Gb/s Surface-Mount PIN/TIA Detector
3 x A$0.00 = A$0.00Optical Fiber Splicing Protector - Heat Shrinkable
1 x A$61.39 = A$61.39Semiconductor Optical Amplifier (SOA) - High Power
1 x A$0.00 = A$0.00Polarization Maintaining (PM) Optical Coupler - 2 micron meter
1 x A$3,075.46 = A$3,075.46Optical Fiber Identifier
1 x A$1,369.26 = A$1,369.26Visual Fiber Fault Finder - 10mW
1 x A$121.54 = A$121.54Optical Fiber Fusion Splicer
1 x A$7,677.11 = A$7,677.11EPON OLT Optical Transceiver - 1.25Gbps SFF Module
1 x A$453.86 = A$453.86Mini Broadband ASE Light Source - 1060nm
1 x A$11,538.75 = A$11,538.75Variable Optical Attenuators - Adapter Type
1 x A$30.75 = A$30.75Gain Flattening Filter for Optical Amplifiers
1 x A$538.47 = A$538.4740-Channel 100GHz Athermal AWG Module
1 x A$1,984.66 = A$1,984.66Optical Source DFB 1310nm
1 x A$3,153.92 = A$3,153.92Uncooled 1310nm SLED Diode - Coaxial Pigtailed
1 x A$460.01 = A$460.0110Gb/s Pluggable SFP+ Transceiver - 1310nm 10km
1 x A$183.08 = A$183.08DWDM DFB Optical Laser Source
1 x A$5,692.45 = A$5,692.45Handheld Variable Optical Attenuator - 850 or 1310nm MMF
1 x A$1,383.11 = A$1,383.11Super Wide Spectrum Light Source - SLED
1 x A$0.00 = A$0.00- A$53,753.48
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Optical Fiber Mirror - Faraday Rotator [FRM]
A$112.16A$101.54-
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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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