Page 267 - Optical Communications Essentials
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Performance Impairments



                                                                    Performance Impairments  257


                                 Interaction up to 125 nm
                                Peak Stokes shift (90 nm)
                                                          Gain peak
                       Relative amplitude  gain curve  Input signal
                                     Raman


                                             @ 1610 nm



                           Input signal  SRS-generated signal
                           @ 1530 nm    @ 1610 nm
                      Figure 15.6. As a result of SRS, the signal at 1530nm acts as
                      a pump for the signal at 1610nm.



                        In general, if the optical power per channel is not excessively high (e.g., less
                      than 1mW each), then the effects of SRS do not contribute significantly to the
                      eye closure penalty as a function of transmission distance. Furthermore, since
                      the generated wavelength is around 90nm away from the signal wavelength,
                      crosstalk from SRS is not a significant problem unless the system operates over
                      a wide spectral range. As an example, consider a WDM system that operates over
                      both the C-band and the L-band (from 1530 to 1620nm). As shown in Fig. 15.6 for
                      two specific wavelengths in this range, as a result of SRS the signal at 1530nm
                      acts as a pump for the signal at 1610nm.

          15.5.3. Stimulated Brillouin scattering
                      Stimulated Brillouin scattering arises when light waves scatter from acoustic
                      waves. The resultant scattered wave propagates principally in the backward
                      direction in single-mode fibers. This backscattered light experiences gain from
                      the forward-propagating signals, which leads to depletion of the signal power.
                      The frequency of the scattered light experiences a Doppler shift given by

                                                          2nV s
                                                     ν B                                (15.7)
                                                           λ
                      where n is the index of refraction and V s is the velocity of sound in the material.
                      In silica this interaction occurs over a very narrow  Brillouin linewidth of
                      ∆ν B   20MHz at 1550nm. For V s   5760m/s in fused silica, the frequency of
                      the backward-propagating light at 1550nm is downshifted by 11GHz (0.09nm)
                      from the original signal. This shows that the SBS effect is confined within a sin-
                      gle wavelength channel in a WDM system. Thus, the effects of SBS accumulate
                      individually for each channel, and consequently they occur at the same power level
                      in each channel as occurs in a single-channel system.


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