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.