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Nonlinear Fiber Optics - 4 ed. Agrawal

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20 Chapter 1. Introduction<br />

Chapters 11 and 12 focus on highly nonlinear fibers develop<strong>ed</strong> during the 1990s.<br />

Various techniques us<strong>ed</strong> to measure the nonlinear parameter are describ<strong>ed</strong> first in Chapter<br />

11. The remainder of this chapter then focuses on four types of highly nonlinear<br />

fibers and their properties. The focus of Chapter 12 is on the novel nonlinear effects<br />

that have become possible with the advent of such fibers. After discussing intrapulse<br />

Raman scattering and FWM, the chapter focuses on supercontinuum generation. The<br />

last section is devot<strong>ed</strong> to second- and third-harmonic generation in optical fibers.<br />

Problems<br />

1.1 Calculate the propagation distance over which the inject<strong>ed</strong> optical power is r<strong>ed</strong>uc<strong>ed</strong><br />

by a factor of two for three fibers with losses of 0.2, 20, and 2000 dB/km.<br />

Also calculate the attenuation constant α (in cm −1 ) for the three fibers.<br />

1.2 A single-mode fiber is measur<strong>ed</strong> to have λ 2 (d 2 n/dλ 2 )=0.02 at 0.8 μm. Calculate<br />

the dispersion parameters β 2 and D.<br />

1.3 Calculate the numerical values of β 2 (in ps 2 /km) and D [in ps/(km-nm)] at 1.5 μm<br />

when the modal index varies with wavelength as n(λ)=1.45 − s(λ − 1.3 μm) 3 ,<br />

where s = 0.003 μm −3 .<br />

1.4 For silica fiber dop<strong>ed</strong> with 7.9% of germania, parameters appearing in the Sellmeier<br />

equation have the following values [69]: B 1 = 0.7136824, B 2 = 0.4254807,<br />

B 3 = 0.8964226, λ 1 = 0.0617167 μm, λ 2 = 0.1270814 μm, and λ 3 = 9.896161<br />

μm. Plot n, n g , and β 2 in the wavelength range of 0.5 to 1.6 μm and comment<br />

on changes from values shown in Figures 1.4 and 1.5.<br />

1.5 Using the parameter values given in the prec<strong>ed</strong>ing problem, calculate the values<br />

of third- and fourth-order dispersion parameters (β 3 and β 4 ) at the zerodispersion<br />

wavelength λ D of the fiber. Calculate β 2 and D when the input wavelength<br />

exce<strong>ed</strong>s λ D by 10 nm.<br />

1.6 A 1-km-long single-mode fiber with the zero-dispersion wavelength at 1.4 μm<br />

is measur<strong>ed</strong> to have D = 10 ps/(km-nm) at 1.55 μm. Two pulses from Nd:YAG<br />

lasers operating at 1.06 and 1.32 μm are launch<strong>ed</strong> simultaneously into the fiber.<br />

Calculate the delay in the arrival time of the two pulses at the fiber output assuming<br />

that β 2 varies linearly with wavelength over the range 1.0–1.6 μm.<br />

1.7 Define the dispersion parameters D and β 2 and derive a relation between the two.<br />

Prove that D = −(λ/c)(d 2 n/dλ 2 ).<br />

1.8 Explain the concepts of birefringence and beat length. Why does an optical fiber<br />

exhibit some residual birefringence that varies randomly along its length?<br />

1.9 What is meant by polarization-mode dispersion in the context of optical fibers?<br />

What happens to optical pulses when a fiber exhibits randomly varying birefringence<br />

along its length?<br />

1.10 Sketch a design for a polarization-maintaining fiber. Under what conditions do<br />

such fibers maintain polarization? What happens to the state of polarization<br />

when input light is polariz<strong>ed</strong> linearly at an angle of 10 ◦ from the slow axis of the<br />

fiber?

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