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Fiber Optis can be used in so many fields:

 

  • Data Storage Equipment

  • Interconnects,Networking

  • Gigabit Ethernet

  • FTTx, HDTV,CATV

  • Aerospace & Avionics

  • Data Transfer Tests

  • Network Equipment

  • Broadcast Automotive

  • Electronics,Sensing

  • Oil & Gas, Imaging

  • Outside Plant,Central Office

  • Harsh Environment

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  • Illumination,Institutions

  • Ship to Shore,Education

  • Simulation,Military,Space

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  • Semiconductor Equipment

  • Diagnostics & Troubleshooting

  • Premise Networks Carrier Networks

  • Independent Telecommunication Providers

 

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Info about Fiber Optic Bandwidth

 

 

Multimode fiber's information transmission capacity is limited by two separate components of dispersion: modal and chromatic. Modal dispersion comes from the fact that the index profile of the multimode fiber isn't perfect. The graded index profile was chosen to theoretically allow all modes to have the same group velocity or transit speed along the length of the fiber. By making the outer parts of the core a lower index of refraction than the inner parts of the core, the higher order modes speed up as they go away from the center of the core, compensating for their longer path lengths.

 

Modal Dispersion

Modal Dispersion

 

In an idealized fiber, all modes have the same group velocity and no modal dispersion occurs. But in real fibers, the index profile is a piecewise approximation and all modes are not perfectly transmitted, allowing some modal dispersion.

 

Since the higher order modes have greater deviations, the modal dispersion of a fiber (and therefore its laser bandwidth) tends to be very sensitive to modal conditions in the fiber. Thus the bandwidth of longer fibers degrades nonlinearly as the higher order modes are attenuated more strongly.

 

Chromatic Dispersion

Chromatic Dispersion

 

The second factor in fiber bandwidth, chromatic dispersion, affects both multimode and single mode fiber. Remember a prism spreads out the spectrum of incident light since the light travels at different speeds according to its color and is therefore refracted at different angles. The usual way of stating this is the index of refraction of the glass is wavelength dependent. Thus a carefully manufactured graded index profile can only be optimized for a single wavelength, usually near 1300 nm, and light of other colors will suffer from chromatic dispersion. Even light in the same mode will be dispersed if it is of different wavelengths.

 

Light Source

Light Source

 

Chromatic dispersion is a big problem with LED sources in MM fiber, which have broad spectral outputs, unlike lasers which concentrate most of their light in a narrow spectral range. Systems like FDDI, based on broad spectral output surface emitter LEDs, suffered such intense chromatic dispersion that transmission was limited to only two km of 62.5/125 fiber.

 

Chromatic dispersion (CD) also affects long links in single mode systems, even with lasers, so fiber and sources are optimized to minimize chromatic dispersion in the long distance links.

 

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