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4 hours ago comment added TimWescott You don't have to just make the claim that $\mathcal F \left \{ e^{j 2 \pi f t} \right \} = \delta(\omega - 2 \pi f)$ and then backfill by showing it makes sense. You can time-limit the exponential to a rectangular pulse of duration $T$, or you can multiply it by a $\mathrm{sinc} \frac t T$, then find that in the limit as $T \to \infty$ you end up with something that acts like $\delta (\omega - 2 \pi f)$. It's a good exercise if you're feeling like the Fourier transform of a continuous sine wave isn't philosophically valid.
10 hours ago history answered Marcus Müller CC BY-SA 4.0