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Nonlinear Fiber Optics - 4 ed. Agrawal

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Chapter 12<br />

Novel <strong>Nonlinear</strong> Phenomena<br />

The development of highly nonlinear fibers discuss<strong>ed</strong> in Chapter 11 has l<strong>ed</strong> to the observation<br />

of novel nonlinear effects such as the generation of extremely broad optical<br />

spectra (supercontinuum generation) and large Raman-induc<strong>ed</strong> frequency shifts that allow<br />

wavelength tuning of mode-lock<strong>ed</strong> lasers. These nonlinear phenomena are finding<br />

a multitude of new applications for optical fibers in fields as diverse as high-precision<br />

metrology and optical coherence tomography. This chapter focuses on several nonlinear<br />

effects that have been attracting attention in recent years. We revisit in Section<br />

12.1 the topic of Raman-induc<strong>ed</strong> frequency shifts discuss<strong>ed</strong> earlier in Section 5.5. It<br />

turns out that such spectral shifts can be enhanc<strong>ed</strong> as well as suppress<strong>ed</strong> with a proper<br />

design of highly nonlinear fibers. Section 12.2 discusses how dispersion tailoring in<br />

highly nonlinear fibers can be us<strong>ed</strong> to enhance the four-wave mixing (FWM) effects<br />

for practical applications. Supercontinuum generation is cover<strong>ed</strong> in Section 12.3 with<br />

emphasis on the physical processes behind its creation. Section 12.4 focuses on the<br />

temporal, spectral, polarization, and coherence properties of a supercontinuum and<br />

employs numerical simulations to understand the underlying physics. Section 12.5<br />

is devot<strong>ed</strong> to the topic of harmonic generation in optical fibers with emphasis on the<br />

second and third harmonics.<br />

12.1 Intrapulse Raman Scattering<br />

As discuss<strong>ed</strong> in Section 5.5.4, the spectrum of an ultrashort pulse shifts toward longer<br />

wavelengths because of intrapulse Raman scattering. Such a shift was first notic<strong>ed</strong><br />

around 1985 in the context of solitons and was call<strong>ed</strong> the soliton self-frequency shift<br />

[1]. The term Raman-induc<strong>ed</strong> frequency shift (RIFS) was us<strong>ed</strong> in Section 4.4.3 because<br />

a spectral shift can occur even in the normal-GVD regime of an optical fiber where<br />

solitons are not form<strong>ed</strong> [2]. It was discover<strong>ed</strong> during the 1990s that the RIFS of solitons<br />

can become quite large in highly nonlinear fibers. Later experiments reveal<strong>ed</strong> that it<br />

can also be suppress<strong>ed</strong> under certain conditions. This section focuses on such novel<br />

aspects of intrapulse Raman scattering.<br />

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