MisterX
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From what I have seen, Fermi's Golden rule is applied to constant or sinusoidal time varying potentials. But what if the perturbation is of the form V_0\left( \mathbf{x}\right)f\left(t\right), where f(t) is not a constant or sinusoidal? I am not really familiar with the derivation of Fermi's golden rule, and the explanations I was given both seemed very hand-wavy. I know we can Fourier decompose f(t) in time, but it's not clear to me how that might be related back to transition probabilities. In particular, what if f(t) = e^{-a t} with a \in \mathbb{R}, a > 0 ?