The relation implies . Fix and split the Riesz potential into the regions and .
For the near part, decompose the ball into the dyadic annuli
The definition of the Hardy-Littlewood maximal function then gives
For the far part, Hölder's inequality gives
where convergence follows from .
If , choose
The two bounds then have the same size. If , the result is immediate. Consequently the Hedberg inequality is
Here the dimensional constant is required for the unnormalized kernel and Lebesgue measure used in the question.