12:43 AM
Anyway, the point of all of this is that if we rewrite our differential equation in the $\omega$ basis we get:
2 hours later…
3:09 AM
In this example where we have a damped driven harmonic oscillator, $J(t)$ would be something like a voltage or current drive.
For example, we could inject a probe signal $J(t)$ into our system and then measure how the system responds.
Note that if $J$ is sinusoidal, then $\tilde{J}(\omega)$ is a delta function (or pair of delta functions, one for positive and one for negative frequency).
1 hour later…
4:57 AM
15 hours later…
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