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Nonlinear Fiber Optics - 4 ed. Agrawal

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Problems 321<br />

Figure 8.25: (a) Average gain and (b) standard deviation of signal fluctuations at the output of a<br />

Raman amplifier as a function of PMD parameter in the cases of forward and backward pumping.<br />

The solid and dash<strong>ed</strong> curves correspond to the cases of copolariz<strong>ed</strong> and orthogonally polariz<strong>ed</strong><br />

signals, respectively. (After Ref. [189]; c○2003 OSA.)<br />

The level of signal fluctuations in Figure 8.25 increases quickly with the PMD<br />

parameter, reaches a peak value, and then decreases slowly toward zero with a further<br />

increase in D p because of an averaging effect produc<strong>ed</strong> by the PMD. The location of the<br />

peak depends on the pumping scheme as well as on the initial polarization of the pump;<br />

the noise level near this peak exce<strong>ed</strong>s 40%. If a fiber with low PMD is us<strong>ed</strong>, the noise<br />

level can exce<strong>ed</strong> 70% under some operating conditions. The behavior for backward<br />

pumping is similar to those for forward pumping but the peak shifts to smaller D p<br />

values. This shift is due to a much larger value of |Ω| = ω p + ω s . Since the diffusion<br />

length scales as |Ω| −2 , it is smaller by about a factor of (ω p + ω s )/(ω p − ω s ) ≈ 30 in<br />

the backward-pumping case. A smaller diffusion length results in rapid averaging over<br />

birefringence fluctuations and r<strong>ed</strong>uces the noise level.<br />

An important question is which pumping configuration is better from a practical<br />

viewpoint. The answer depends on the value of D p . For fibers with values of D P <<br />

0.001 ps/ √ km, forward pumping is the appropriate choice. However, D p exce<strong>ed</strong>s 0.01<br />

ps/ √ km for most fibers. In this situation, backward pumping produces the least signal<br />

degradation in practice. It also r<strong>ed</strong>uces the polarization dependence of the Raman gain<br />

in optical communication systems where the SOP of the input signal itself may change<br />

with time in a random fashion.<br />

Problems<br />

8.1 What is meant by Raman scattering? Explain its origin. What is the difference<br />

between spontaneous and stimulat<strong>ed</strong> Raman scattering?<br />

8.2 Solve Eqs. (8.1.2) and (8.1.3) neglecting pump deletion. Calculate the Stokes<br />

power at the output of a 1-km-long fiber when 1-μW power is inject<strong>ed</strong> together

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