Take a function $f$ then and use the following definition of Fourier transform $\mathcal{F}$: $$\mathcal{F}(f)(\xi) = \hat{f}(\xi)=\int_{-\infty}^{\infty} f(x) e^{-i \xi x} d x, \quad \forall \xi \in \mathbb{R} $$ One can prove that taking the Fourier transform twice leads to: $$\mathcal{F}^2(f)(x) = 2 \pi f(-x)$$ a proof of this fact can be found at this post Fourier transform of the Fourier transform.
However now I am interested in Fourier transforms of probability measures. We know that if we let $\mu$ be a probability measure on $(\mathbb{R}, \mathcal{B})$. Its characteristic function $\phi: \mathbb{R} \rightarrow \mathbb{C}$ is defined by $$ \phi(u)=\int_{\mathbb{R}} e^{\mathrm{i} u x} \mu(\mathrm{d} x) $$
Now if we let the $f$ from above to be the density of $\mu$ then we see the equality: $$\phi(u)=\hat{f}(-u)$$ Then we can play the same game as above and see that if we take again the Fourier we obtain again the density $f$ times $2 \pi$. But what happens if $\mu$ does not admit density?
Q: What object do we get if we take twice the Fourier transform of a probability measure that does not admit density?