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Nonlinear Fiber Optics - 4 ed. Agrawal

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12.1. Intrapulse Raman Scattering 455<br />

Figure 12.1: Left Panel: Measur<strong>ed</strong> (a) spectrum and (b) autocorrelation trace of the Raman<br />

soliton at the output of a taper<strong>ed</strong> fiber. Right Panel: Numerically simulat<strong>ed</strong> (a) evolution of pulse<br />

spectrum and (b) output spectrum. Dash<strong>ed</strong> curves show the input spectrum. (After Ref. [13];<br />

c○2001 OSA.)<br />

damental solitons of different widths and peak powers. The inverse scattering method<br />

(see Section 5.2.1) shows that their widths and peak powers are relat<strong>ed</strong> to N as [6]<br />

T k =<br />

T 0<br />

2N + 1 − 2k , P (2N + 1 − 2k)2<br />

k =<br />

N 2 P 0 , (12.1.2)<br />

where k = 1to ¯N. As an example, when N = 2.1, two fundamental solitons creat<strong>ed</strong><br />

through the fission process have widths of T 0 /3.2 and T 0 /1.2. The narrower soliton<br />

exhibits a much larger RIFS compar<strong>ed</strong> with the broader one because of the T0 −4 dependence<br />

seen in Eq. (12.1.1). For the N = 2.1 example, the enhancement factor for<br />

the narrower soliton is about 105. Figure 12.1 agrees with this scenario as the Raman<br />

soliton, whose spectrum has been shift<strong>ed</strong> by 250 nm, has a width of 62 fs, about 3.3<br />

times smaller than the input pulse width of 205 fs. Numerical simulations reveal that<br />

fission occurs within 2 cm of propagation inside the taper<strong>ed</strong> fiber. The spectrum of the<br />

ultrashort soliton shifts rapidly toward the r<strong>ed</strong> side, as dictat<strong>ed</strong> by Eq. (12.1.1). After<br />

15 cm, the spectrum has shift<strong>ed</strong> to near 1550 nm. This pr<strong>ed</strong>ict<strong>ed</strong> behavior agrees with<br />

the experimental data qualitatively.<br />

A 60-cm-long photonic crystal fiber having its zero-dispersion wavelength (ZDWL)<br />

at 690 nm was us<strong>ed</strong> in a 2002 experiment [16]. Figure 12.2 shows the experimentally<br />

measur<strong>ed</strong> output spectra at several average power levels when 70-fs pulses with a 48-<br />

MHz repetition rate at a wavelength of 782 nm were launch<strong>ed</strong> into this fiber. After<br />

the input power exce<strong>ed</strong>s a value large enough to ensure N > 1, a Raman soliton is<br />

generat<strong>ed</strong>, and its wavelength shifts continuously through RIFS inside the fiber. The<br />

total shift at the output of fiber becomes larger as the input power is increas<strong>ed</strong>. The

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