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

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11<br />

for materials with no free charge. This implies<br />

V'. E(w) = _ 47rV' . P(2)(W).<br />

€(w)<br />

(2.7)<br />

2.2 Properties <strong>of</strong> X~~k(w = 2wo)<br />

A full expression for the second-order susceptibility element that describes secondharmonic<br />

generation is<br />

+ (1Ir,ln)(nlr.lm)(mlrk II)<br />

[(W-Wmn )+hmn][(Wo+Wnl )-hnl J<br />

+ (1Ir,ln)(nlr;lm)(mlrkll)<br />

[(W+Wnm )-hnm ][(wo -Wml )+hml J<br />

+ (1Ir,ln)(nlrklm)(mlr.II») (? 8)<br />

[(w+wmd-t"fmd[(wo+wnd+hnd . _.<br />

Equation (2.8) can be derived from first principles using quantum statistical mechanics<br />

with the proper choice <strong>of</strong> the interaction Hamiltonian [34]. In equation (2.8)<br />

It), 1m), <strong>and</strong>ln) are quantum mechanical states <strong>of</strong> the system; pf?) is the unperturbed<br />

density <strong>of</strong> the state It), i.e. p(O) is the equilibrium population distribution: -eri is<br />

the dipole moment operator along direction i; liw nm is the energy difference between<br />

states In) <strong>and</strong> 1m); <strong>and</strong> 'Ynm is a dephasing term. The different terms in equation<br />

(2.8) correspond to different time ordering <strong>of</strong> the photons. This is discussed further<br />

in section 5.-1.1.<br />

There are a few salient features <strong>of</strong> equation (2.8) that bear discussion.<br />

First.<br />

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