Given a continuous function $f:\mathbb{R}\to\mathbb{R}$, with either $f(t)$ or $f(-t)$ diverging to $\pm\infty$ as $t\to\infty$, is there a way to define its Fourier transform in a way that conserves $$\mathcal{F}^{-1}\left\{\mathcal{F}_{\mathfrak{R}}\{f(t)\}_s\right\}_{t}=f(t)$$ For some non-degenerate interval of $t$?
As the usual integral definition lacks the capacity to control a function's growth like Laplace, Mellin or even Hillbert transforms.
The closest I have found is for $f\left(e^{-t}\right)$ with an inverse $f^{-1}(t)$ defined for $t\in f\left(\mathbb{R}^+\right)$, a semi-regularization: $$\mathcal{F}\left\{f\left(e^{-t}\right)\right\}_s=\frac{i}{s}\int_{f\left(\mathbb{R}^+\right)}f^{-1}(t)^{is}dt$$ Which doesnt converge by itself, needs either weight functions or a Wick rotation.
Its a re-formulation of the Mellin-Fourier duality: $$\mathcal{F}\left\{f\left(e^{-t}\right)\right\}_{-is}=\mathcal{M}\{f\}_s$$ But this one only works if $f$ grows as a power of $x$, and doesnt allow exponential or higher growth as the semi-regularization.