The Riesz potential of order is the integral operator
defined whenever the integral converges, where is the Euclidean
norm. It is a convolution with a power-law integral kernel. The normalization constant
is chosen so that, for
a Schwartz function
and the Fourier transform
convention using
, its Fourier
multiplier is
, with the identity
understood in the sense of generalized functions.
For
with
and
, this is the inverse potential associated with
the fractional Laplacian (Mei and Wei 2026).