- #1
Judas503
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Homework Statement
The problem requires to solve the integration to find ## G(t) ## after ##G(\omega)## is found via Fourier transform. We have [tex] G(\omega)= \frac{1}{2\pi}\frac{1}{\omega _{0}^2 - \omega ^2}[/tex]
Homework Equations
As mentioned previously, the question asks to find ##G(t)##
The Attempt at a Solution
It is obvious that calculus of residues is required. To account for causality (## G(t<0)=0 ##), the poles at ## \omega=\pm \omega_{0} ## are shifted to the lower half plane by ## i\epsilon ## and integrated along the contour in the lower half plane. Then,
[tex] G(t)=-\frac{1}{2\pi}\int_{-\infty}^{+\infty}\frac{e^{-i\omega t}}{(\omega +i\epsilon)^2 -\omega _{0} ^2}d\omega [/tex]
After calculating the residues at ## \omega =\pm \omega _{0} - i\epsilon ##, I found
[tex] G(t)=\frac{i}{2\omega_{0}}\sin \omega_{0}t [/tex]
Is my answer correct?