Optical Fiber CommunicationsThe third edition of this popular text and reference book presents the fundamental principles for understanding and applying optical fiber technology to sophisticated modern telecommunication systems.. Optical-fiber-based telecommunication networks have become a major information-transmission-system, with high capacity links encircling the globe in both terrestrial and undersea installations. Numerous passive and active optical devices within these links perform complex transmission and networking functions in the optical domain, such as signal amplification, restoration, routing, and switching. Along with the need to understand the functions of these devices comes the necessity to measure both component and network performance, and to model and stimulate the complex behavior of reliable high-capacity networks. |
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Page 122
... radius a of the fiber core area , Eq . ( 5 - 7 ) becomes Pled , step A ) for r , > a ( 5
- 8 ) In the case of a graded - index fiber , the numerical aperture depends on the
distance r from the fiber axis through the relationship defined by Eq . ( 2 - 62 ) .
... radius a of the fiber core area , Eq . ( 5 - 7 ) becomes Pled , step A ) for r , > a ( 5
- 8 ) In the case of a graded - index fiber , the numerical aperture depends on the
distance r from the fiber axis through the relationship defined by Eq . ( 2 - 62 ) .
Page 192
bandwidth is used as ß decreases , the tails of hour ( t ) become larger , and
signal timing and equalization become more ... impulse input H ( 0 ) and a raised
cosine output , 1x = Le Huc6b ) dob = 1 - ( 7 - 62 ) which , for ß = 1 , becomes ( 7 -
63 ) ...
bandwidth is used as ß decreases , the tails of hour ( t ) become larger , and
signal timing and equalization become more ... impulse input H ( 0 ) and a raised
cosine output , 1x = Le Huc6b ) dob = 1 - ( 7 - 62 ) which , for ß = 1 , becomes ( 7 -
63 ) ...
Page 249
Since this becomes increasingly difficult as the fiber becomes longer ( because of
the feebleness of the back - scattered light ) , a photoncounting technique has
been devised . " The details of this method are beyond the scope of this book ,
but ...
Since this becomes increasingly difficult as the fiber becomes longer ( because of
the feebleness of the back - scattered light ) , a photoncounting technique has
been devised . " The details of this method are beyond the scope of this book ,
but ...
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Contents
Structures and Waveguiding | 12 |
Signal Degradation in Optical Fibers | 48 |
Optical Sources | 80 |
Copyright | |
9 other sections not shown
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Common terms and phrases
absorption active addition amplifier angle applications approximately arise assume attenuation avalanche band bandwidth becomes bias cable carrier characteristics cladding communication components condition consider constant core coupling defined density depends detector determined device dispersion distance distortion effects efficiency electric Electron emitting energy equal equation example expression factor field Figure frequency function gain given gives glass graded-index guided IEEE important increases input laser diodes length less light limit loss material measured mechanical method modes modulation noise occurs operating optical fiber optical power optical source output parameter percent photodetector photodiode photon propagation pulse quantum range ratio receiver referred reflection region respectively response rise shown in Fig signal spectral surface technique temperature transmission transmitter values various voltage wave waveguide wavelength width York