29.03.2016 Views

Nonlinear Fiber Optics - 4 ed. Agrawal

You also want an ePaper? Increase the reach of your titles

YUMPU automatically turns print PDFs into web optimized ePapers that Google loves.

9.1. Basic Concepts 331<br />

Figure 9.1: Brillouin-gain spectra of three fibers for λ p = 1.525 μm: (a) silica-core fiber, (b)<br />

depress<strong>ed</strong>-cladding fiber, and (c) dispersion-shift<strong>ed</strong> fiber. (After Ref. [17]; c○1986 IEE.)<br />

phonon lifetime. As shown later in Section 9.4.1, when acoustic waves decay as<br />

exp(−Γ B t), the Brillouin gain has a Lorentzian spectrum of the form [10]<br />

g B (Ω)=<br />

g p (Γ B /2) 2<br />

(Ω − Ω B ) 2 +(Γ B /2) 2 , (9.1.4)<br />

where the peak value of the Brillouin gain at Ω = Ω B is given by<br />

g p ≡ g B (Ω B )=<br />

8π 2 γ 2 e<br />

n p λ 2 pρ 0 cv A Γ B<br />

. (9.1.5)<br />

Here, γ e ≈ 0.902 is the electrostrictive constant of silica and ρ 0 ≈ 2210 kg/m 3 is its<br />

density [12]. The full width at half maximum (FWHM) of the gain spectrum is relat<strong>ed</strong><br />

to Γ B as Δν B = Γ B /(2π). The phonon lifetime, T B = Γ −1<br />

B<br />

, is typically

Hooray! Your file is uploaded and ready to be published.

Saved successfully!

Ooh no, something went wrong!