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Nonlinear Fiber Optics - 4 ed. Agrawal

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11.1. <strong>Nonlinear</strong> Parameter 433<br />

when pulse width is 100 ns), h a (t) can be replac<strong>ed</strong> with a delta<br />

function. The acoustic contribution then attains its maximum value, and the total n 2 is<br />

close to 2.76 × 10 −20 m 2 /W.<br />

It is clear from the prec<strong>ed</strong>ing discussion that the largest value of n 2 is expect<strong>ed</strong> for<br />

measurements perform<strong>ed</strong> using CW beams or long optical pulses. The XPM technique<br />

has been us<strong>ed</strong> to study the frequency dependence of the electrostrictive contribution<br />

by changing the pump-modulation frequency from 10 MHz to 3 GHz [34]. As seen in<br />

Table 11.1, the measur<strong>ed</strong> value is 2.73 × 10 −20 m 2 /W at 10 MHz (pulse width 100 ns)<br />

but is r<strong>ed</strong>uc<strong>ed</strong> to 2.23 × 10 −20 m 2 /W when the modulation frequency is increas<strong>ed</strong> to<br />

2.3 GHz (pulse width

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