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Nonlinear Fiber Optics - 4 ed. Agrawal

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6.3. Evolution of Polarization State 189<br />

Figure 6.4: Transmittivity T p as a function of input polarization angle θ when the effect of linear<br />

birefringence is includ<strong>ed</strong> for ΔβL = 2π and φ max = 6.5π. Dash<strong>ed</strong> line shows the behavior when<br />

Δβ = 0. (After Ref. [31]; c○1985 AIP.)<br />

components are excit<strong>ed</strong> with equal amplitudes. In practice, this is not the case. The<br />

reason for this discrepancy can be trac<strong>ed</strong> back to the neglect of the last term in Eqs.<br />

(6.1.11) and (6.1.12). A more accurate theory should include this term. In the CW<br />

or the quasi-CW case for which the dispersive effects are negligible, Eqs. (6.1.11) and<br />

(6.1.12) can be solv<strong>ed</strong> analytically by neglecting the time derivatives and the loss terms.<br />

The analytic solution is given in the next section. Its use shows that Eq. (6.2.18) is quite<br />

accurate in the case of highly birefringent fibers (ΔβL ≫ 1) except near θ = 45 ◦ .In<br />

low-birefringence fibers, the transmittivity can be quite different than that given by<br />

Eq. (6.2.18). Figure 6.4 shows T p as a function of θ for ΔβL = 2π and φ max = 6.5π.<br />

A comparison with the pr<strong>ed</strong>iction of Eq. (6.2.18) reveals the importance of including<br />

linear birefringence. Physically, the linear and nonlinear birefringence contributions to<br />

the refractive index compete with each other, and both should be includ<strong>ed</strong>.<br />

6.3 Evolution of Polarization State<br />

An accurate description of the nonlinear polarization effects in birefringent fibers requires<br />

simultaneous consideration of both the modal birefringence and self-induc<strong>ed</strong><br />

nonlinear birefringence [31]–[48]. Evolution of the two polarization components along<br />

such fibers is govern<strong>ed</strong> by Eqs. (6.1.11) and (6.1.12) or their variants. However, before<br />

turning to the case of pulse propagation, it is useful to consider how the state of polarization<br />

evolves within the fiber when a CW (or quasi-CW) beam is launch<strong>ed</strong> at the<br />

input end.<br />

6.3.1 Analytic Solution<br />

In place of Eqs. (6.1.11) and (6.1.12), it is more convenient to use Eqs. (6.1.15) and<br />

(6.1.16) written in terms of the circularly polariz<strong>ed</strong> components. The terms containing

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