Both kernels are integrable functions, so the convolution theorem gives
The uniqueness of the Fourier transform on integrable functions gives equality almost everywhere. Both sides are continuous, so it holds at every point:
For completeness, continuity of the convolution follows by dominated convergence: is bounded and continuous, so for the integrands converge pointwise and are dominated by .
The identity is the heat semigroup property: evolving for time , then for time , is the same as evolving once for time .

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