Solution
= Solution
For the stated <Fourier transform> convention, <Fourier inversion> is
$$
\boxed{f(x)=\frac1{2\pi}\int_{-\infty}^{\infty}\widetilde f(k)e^{ikx}\,dk.}
$$
For example, the pointwise formula holds at continuity points under the usual integrability hypotheses; the same normalization applies to the $L^2$ or distributional inverse.