Formally,
if
is a real- or complex-valued
-periodic function,
The series (1.8.1) is called the Fourier series of
,
and
are the Fourier coefficients of
.
If
, then
for all
.
If
, then
for all
.
where
is square-integrable on
and
are given
by (1.8.2), (1.8.4). If
is also square-integrable
with Fourier coefficients
or
then
If
is of period
, and
is piecewise continuous,
then

If
and
are continuous, have the same period and same Fourier
coefficients, then
for all
.

As ![]()
see Frenzen and Wong (1986).
For
piecewise continuous on
and real
,
as (1.8.10) continues to apply if either
or
or both are
infinite and/or
has finitely many singularities in
, provided
that the integral converges uniformly (§1.5(iv)) at
, and
the singularities for all sufficiently large
.
Let
be an absolutely integrable function of period
, and
continuous except at a finite number of points in any bounded interval. Then
the series (1.8.1) converges to the sum
at every point at which
has both a left-hand derivative (that is,
(1.4.4) applies when
) and a right-hand derivative
(that is, (1.4.4) applies when
). The convergence is
non-uniform, however, at points where
; see
§6.16(i).
For other tests for convergence see Titchmarsh (1962b, pp. 405–410).
If
and
are the Fourier coefficients of a piecewise continuous
function
on
, then

If a function
is periodic, with period
, then the series obtained by differentiating the Fourier series for
term by term converges at every point to
.
Suppose that
is twice continuously differentiable and
and
are integrable over
. Then
It follows from definition (1.14.1) that the integral in (1.8.14)
is equal to
.
An alternative formulation is as follows. Suppose that
is continuous and
of bounded variation on
. Suppose also that
is integrable on
and
as
. Then
As a special case
