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William Angerer - Department of Physics and Astronomy - University ...

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20<br />

nonlinear element <strong>of</strong> quartz, X~~x{w<br />

= 2wo) = 2.2xlO- 9 esu [40]. There are two<br />

solutions to the nonlinear wave equation (equation (2.5)) : a homogeneous solution<br />

<strong>and</strong> a particular solution. vVe refer to the particular solution as the "bound wave·'<br />

solution; the bound wave solution exists only in the nonlinear optical crystal. This<br />

field is bound to the linear field <strong>and</strong> propagates with a wavevector twice that <strong>of</strong> the<br />

linear field. This field may be written as<br />

E - x~E ei (kbl·r--2wot)<br />

b1 - b1 . (2.13 )<br />

The subscript b designates a bound wave solution. The bound wavevector. k bl , is<br />

(2.1.,1)<br />

The magnitude <strong>of</strong> this field is calculated directly from equation (2.5) <strong>and</strong> has a value<br />

<strong>of</strong><br />

47rp(2)<br />

Ebl = --­<br />

Ebl - Ef1<br />

(2.15)<br />

(2.16)<br />

where tOl (w o ) is the Fresnel transmission coefficient for light with angular frequency<br />

;,va which propagates from vacuum into quartz. The homogeneous solution to the<br />

wave equation is<br />

E - x~E ei(k/l·r--2wo t)<br />

/1 - f1 • (2.17)<br />

Reproduced with permission <strong>of</strong> the copyright owner. Further reproduction prohibited without permission.

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