For the stated Fourier transform convention, Fourier inversion is
For example, the pointwise formula holds at continuity points under the usual integrability hypotheses; the same normalization applies to the or distributional inverse.
Assume initially that are integrable, so Fubini's theorem justifies interchanging the integrals. Transform the convolution and put :
This is the convolution theorem. No factor appears in this direction because the forward transform in the question is unnormalized.
Differentiate the defining Fourier integral times with respect to :
For a nonnegative integer , this gives
Integrability of together with suitable lower moments justifies differentiation under the integral. The same multiplication-derivative identity holds more generally for tempered distributions.
Evenness means the negative half of the function is determined as well: this is the triangular function on , zero outside. Its transform is real and even:
Integration by parts, or integrating the two terms separately, gives
The apparent singularity at zero is removable, and its limiting value is the area under . This is the Fourier transform of a triangular function.
Let be the indicator of . The finite integral is exactly the convolution . Its additional transform factor is
Applying the convolution theorem and part (d),
Equivalently this is . The value at zero also follows from .

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