A generalized Fourier series is a series expansion in a complete orthogonal system, with
convergence in the relevant L2-norm.
The prototypical example is the Fourier series
based on the constant function 1 and the functions
and
,
,
on
.
Another example is the Laplace series, a double
series expansion in the spherical
harmonics
.
Their inner product uses complex
conjugation and the area element
over
and
(NIST, §14.30(ii)).
For a complete orthogonal system of nonzero univariate
functions
on an interval
, take a nonnegative measurable
function
as weight. Work in the L2-space
,
identifying functions equal almost
everywhere with respect to
. The orthogonality relationship is
|
(1)
|
where
and
is the Kronecker delta. For
, the expansion
|
(2)
|
means that the partial sums converge to
in norm (Axler 2026, pp. 242-244).
For fixed
and
,
finite summation gives
|
(3)
|
Passing to the limit is justified by Schwarz's inequality, since . Thus the
expansion coefficients are
|
(4)
|
This argument uses finite sums before a norm limit, and does not require interchanging an infinite series and an integral.
A useful special form occurs when the constant function 1 and two families and
together form a complete
orthogonal system in
. Assume
, and write the orthogonality relationships
as
|
(5)
| |||
|
(6)
| |||
|
(7)
| |||
|
(8)
| |||
|
(9)
|
for ,
where
.
Define the finite partial sum
|
(10)
|
For ,
the corresponding calculations are
|
(11)
|
Taking limits in the inner product, as above, gives
|
(12)
| |||
|
(13)
| |||
|
(14)
|
The usual Fourier series is recovered by taking
and
for
,
together with the constant function 1, over
with weight
. For every positive integer
,
|
(15)
| |||
|
(16)
|
Therefore, the Fourier series of a function
is given by
|
(17)
|
where the coefficients are
|
(18)
| |||
|
(19)
| |||
|
(20)
|
A complete biorthogonal system generalizes the coefficient pairing beyond orthogonal functions. Its completeness alone does not assert that the associated series converges in norm to every vector; a Schauder basis requires that additional expansion property (Heil 1998, pp. 50-51).