A Fourier extension operator associated with a surface
and surface measure
is the operator
For integrable ,
this is the inverse Fourier transform of the
measure
.
It is dual to the Fourier restriction
operator under the integral pairing.
For the unit sphere with surface measure
, the constant
function
gives
for , with value
at
.
This example belongs to
for
but fails to belong to
. It explains the strict output exponent in the three-dimensional
Fourier restriction conjecture.