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Nonlinear Fiber Optics - 4 ed. Agrawal

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448 Chapter 11. Highly <strong>Nonlinear</strong> <strong>Fiber</strong>s<br />

Figure 11.20: (a) Cross section of a microstructur<strong>ed</strong> fiber made with tellurite glass; (b) transmission<br />

view observ<strong>ed</strong> with a microscope. (After Ref. [105]; c○2003 OSA.)<br />

nature, bismuth-oxide fibers are being us<strong>ed</strong> for a variety of applications, including<br />

supercontinuum generation [108], a topic we turn to in the next chapter.<br />

Problems<br />

11.1 The refractive index of an optical fiber is specifi<strong>ed</strong> as n = n 0 + n 2 I, where n 0 =<br />

1.45, n 2 = 2.7×10 −20 m 2 /W and I is the optical intensity. If it is written in terms<br />

of the electric field as n = n 0 + n E 2 |E|2 , find the magnitude of n E 2 .<br />

11.2 Light from two CW lasers differing in their wavelengths by a small amount Δλ<br />

is transmitt<strong>ed</strong> through a fiber of length L. Derive an expression for the optical<br />

spectrum at the fiber output after including the effects of SPM-induc<strong>ed</strong> phase<br />

shift. Assume equal input powers for the two lasers and neglect fiber loss and<br />

dispersion for simplicity.<br />

11.3 Explain how the optical spectrum obtain<strong>ed</strong> in the prec<strong>ed</strong>ing problem can be us<strong>ed</strong><br />

to estimate the nonlinear parameter γ. Also, derive the expression for the power<br />

ratio given in Eq. (11.1.5).<br />

11.4 Discuss how the nonlinear phenomenon of XPM can be us<strong>ed</strong> to d<strong>ed</strong>uce γ for an<br />

optical fiber. Why is it important to depolarize the pump light when a pump–<br />

probe configuration is employ<strong>ed</strong>?<br />

11.5 The measur<strong>ed</strong> values of γ are found to be smaller by about 20% when pulses<br />

shorter than 1 ns are employ<strong>ed</strong>. Explain the physical process responsible for this<br />

r<strong>ed</strong>uction. What would happen if femtosecond pulses are employ<strong>ed</strong> for measuring<br />

γ?<br />

11.6 Explain why large values of γ cannot be realiz<strong>ed</strong> by r<strong>ed</strong>ucing the core diameter<br />

of a fiber design<strong>ed</strong> with silica cladding to below 1 μm? Using A eff = πw 2 with<br />

w = a/ √ lnV , prove that the maximum value of γ occurs when the V = √ e,<br />

where V parameter of the fiber is defin<strong>ed</strong> as in Eq. (11.2.1).<br />

11.7 Solve the eigenvalue equation (2.2.8) given in Section 2.2.1 for a taper<strong>ed</strong> fiber<br />

with air cladding using n 1 = 1.45, n 2 = 1, and a = 1 μm and plot β(ω) in the

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