(adsbygoogle = window.adsbygoogle || []).push({}); 1. The problem statement, all variables and given/known data

Hi

I am trying to solve problem 2.1 in these notes (it is on the very first page): http://qis.ucalgary.ca/quantech/673/notes/chapter_two.pdf [Broken]. The problem tells me to show that the Fourier transform of

[tex]

P^{(2)} (t) = \varepsilon _0 \frac{1}{{(2\pi )^2 }}\int_{ - \infty }^\infty {\int_{ - \infty }^\infty {\chi ^{(2)} (t_1 ,t_2 )E(t - t_1 )E(t - t_2 )dt_1 dt_2 } }

[/tex]

is given by

[tex]

P^{(2)}(\omega ) = \varepsilon _0 \int_{ - \infty }^\infty {\int_{ - \infty }^\infty {\chi ^{(2)} (\omega _1 ,\omega _2 )\delta (\omega - \omega _1 - \omega _2 )E(\omega _1 )E(\omega _2 )d\omega _1 d\omega _2 } }

[/tex]

3. The attempt at a solution

OK, so I know that the FT of a convolution yields a product and that the FT of a delta-function is a constant. I am not sure whether to

1) tack on a factor of exp(-iωt) and integrate over t on both sides OR

2) write every factor in terms of its FT, and then compare terms in the end

I choose option 2. Here goes

[tex]

\int_{ - \infty }^\infty {P(\omega )e^{ - i\omega t} } = \varepsilon _0 \frac{1}{{(2\pi )^2 }}\int_{ - \infty }^\infty {\int_{ - \infty }^\infty {\chi ^{(2)} (\omega _1 ,\omega _2 )e^{ - i\omega _1 t_1 - i\omega _2 t_2 } E(\omega _1 )e^{ - i\omega _1 (t - t_1 )} E(\omega _2 )e^{ - i\omega _2 (t - t_2 )} d\omega _1 d\omega _2 dt_1 dt_2 } }

[/tex]

But this makes t_{1}and t_{2}go out in the exponentials, which is no good. But if I go back to option 1, I can't see how I would ever end up with a delta-function in ω-ω_{1}-ω_{2}.

I would really appreciate a hint.

Best,

Niles.

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# Second order polarization

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