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Nonlinear Fiber Optics - 4 ed. Agrawal

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Chapter 3<br />

Group-Velocity Dispersion<br />

The prec<strong>ed</strong>ing chapter show<strong>ed</strong> how the combin<strong>ed</strong> effects of group-velocity dispersion<br />

(GVD) and self-phase modulation (SPM) on optical pulses propagating inside a fiber<br />

can be studi<strong>ed</strong> by solving a pulse-propagation equation. Before considering the general<br />

case, it is instructive to study the effects of GVD alone. This chapter considers the<br />

pulse-propagation problem by treating fibers as a linear optical m<strong>ed</strong>ium. In Section 3.1<br />

we discuss the conditions under which the GVD effects dominate over the nonlinear<br />

effects by introducing two length scales associat<strong>ed</strong> with GVD and SPM. Dispersioninduc<strong>ed</strong><br />

broadening of optical pulses is consider<strong>ed</strong> in Section 3.2 for several specific<br />

pulse shapes, including Gaussian and “sech” pulses. The effects of initial frequency<br />

chirping are also discuss<strong>ed</strong> in this section. Section 3.3 is devot<strong>ed</strong> to the effects of thirdorder<br />

dispersion on pulse broadening. An analytic theory capable of pr<strong>ed</strong>icting dispersive<br />

broadening for pulses of arbitrary shapes is also given in this section. Section 3.4<br />

discusses how the GVD limits the performance of optical communication systems and<br />

how the technique of dispersion management can be us<strong>ed</strong> to combat them in practice.<br />

3.1 Different Propagation Regimes<br />

In Section 2.3 we focus<strong>ed</strong> on the nonlinear Schrödinger (NLS) equation that governs<br />

propagation of optical pulses inside single-mode fibers. For pulse widths >5 ps, we<br />

can use Eq. (2.3.45) in the form<br />

i ∂A<br />

∂z = −iα 2 A + β 2 ∂ 2 A<br />

2 ∂T 2 − γ|A|2 A, (3.1.1)<br />

where A is the slowly varying amplitude of the pulse envelope and T is measur<strong>ed</strong> in<br />

a frame of reference moving with the pulse at the group velocity v g (T = t − z/v g ).<br />

The three terms on the right-hand side of Eq. (3.1.1) govern, respectively, the effects<br />

of fiber losses, dispersion, and nonlinearity on pulses propagating inside optical fibers.<br />

Depending on the initial width T 0 and the peak power P 0 of the incident pulse, either<br />

dispersive or nonlinear effects may dominate along the fiber. It is useful to introduce<br />

51

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