Let
be a function defined on an open interval
, which can be
infinite. The closure of the set of points where
is called the
support of
. If the support of
is a compact set
(§1.9(vii)), then
is called a function of compact
support. A test function is an infinitely differentiable function of
compact support.
A sequence
of test functions converges
to a test function
if the support of every
is contained in a
fixed compact set
and as
the sequence
converges uniformly on
to
for
.
The linear space of all test functions with the above definition of convergence
is called a test function space. We denote it by
.
A mapping
is a linear functional
if
where
and
are real or complex constants.
is called a distribution,
or generalized function,
if it is a continuous linear functional on
, that is, it is a
linear functional and for every
in
,
From here on we write
for
. The
space of all distributions will be denoted by
. A
distribution
is called regular
if there is a locally integrable function
on
(i.e., a function
on
which is absolutely Lebesgue integrable
on every compact subset of
) such that
We denote a regular distribution by
, or simply
, where
is
the function giving rise to the distribution. (If a distribution is not
regular, it is called singular.)
More generally, for
a nondecreasing
function the corresponding Lebesgue–Stieltjes measure
(see §1.4(v)) can be considered as a distribution:
Define
where
is a constant. More generally, if
is an infinitely
differentiable function, then
We say that a sequence of distributions
converges
to a distribution
in
if
for all
.
The derivative
of a distribution is defined by

Similarly

If
is a locally integrable function then its distributional derivative
is
.
In the situation of (1.16.3_5) we have
If the measure
is absolutely continuous with density
(see §1.4(v)) then
.
The Dirac delta distribution is singular. See also §1.17(i).
Since
is the Lebesgue–Stieltjes measure
corresponding to
(see §1.4(v)), formula (1.16.16) is a special case of (1.16.3_5), (1.16.9_5) for
that choice of
.
Suppose
is infinitely differentiable except at
, where left and
right derivatives of all orders exist, and
Then
For
,
For
,
For
and
not an integer, define
where
is an integer such that
. Similarly, we write
and define
The space
of test functions for tempered distributions
consists of all infinitely-differentiable functions such that the function and
all its derivatives are
as
for all
.
A sequence
of functions in
is said to
converge to a function
as
if the
sequence
converges uniformly to
on every
finite interval and if the constants
in the inequalities
do not depend on
.
A tempered distribution
is a continuous linear functional
on
. (See the
definition of a distribution in §1.16(i).) The set of tempered
distributions is denoted by
.
A sequence of tempered distributions
converges to
in
if
for all
.
The derivatives of tempered distributions are defined in the same way as derivatives of distributions.
For a detailed discussion of tempered distributions see Lighthill (1958).
Let
be the set of all infinitely
differentiable functions in
variables,
, with
compact support in
. If
is a multi-index and
, then we write
and
.
A sequence
of functions in
converges to a
function
if the supports of
lie in a fixed
compact subset
of
and
converges uniformly to
in
for every multi-index
. A distribution in
is a continuous
linear functional on
.
The partial derivatives of distributions in
can be defined as in
§1.16(ii). A locally integrable function
gives rise to a distribution
defined by

The distributional derivative
of
is defined by

where
is a multi-index and
.
For tempered distributions the space of test functions
is the
set of all infinitely-differentiable functions
of
variables that
satisfy
Here
and
are multi-indices,
and
are constants. Tempered distributions are continuous linear
functionals on this space of test functions. The space of tempered
distributions is denoted by
.
Suppose
is a test function in
. Then its Fourier
transform
is
where
and
.
is also in
.
Let
For a
multi-index
, define
and
Here
ranges over a finite set of multi-indices,
is a multivariate polynomial, and
is a partial differential operator.
Then
and
If
is a tempered distribution,
then its Fourier transform
is defined by


The Fourier transform
of a tempered distribution is again a tempered distribution,
and
in which
; compare (1.16.33) and (1.16.34).
In (1.16.36) and (1.16.37) the derivatives in
are understood to be in the sense of distributions, as defined in §1.16(ii)
and we also use the convention (1.16.6).
Suggested 2017-03-07 by Roderick Wong
We use the notation of the previous subsection and take
and
in (1.16.35). We obtain

As distributions, the last equation reads
which is often written conventionally as
see also (1.17.2).
Since
, we have
in which
.
The second to last equality follows from the Fourier integral formula (1.17.8).
Since the quantity on the extreme right of (1.16.41) is equal to
, as distributions, the result in this equation can be stated as
and conventionally it is expressed as
see also (1.17.12).
It is easily verified that

and from (1.16.15) we find
where
is the Heaviside function defined in (1.16.13),
and the derivatives are to be understood in the sense of distributions.
Then
and from (1.16.36) with
,
, and
, we have also
Coupling (1.16.46) and (1.16.47) gives
that is
The Fourier transform of
now follows from (1.16.42)
and (1.16.48).
Indeed, we have
that is
For more detailed discussions of the formulas in this section, see Kanwal (1983) and Debnath and Bhatta (2015).
See Hildebrandt (1938) and Chihara (1978, Chapter II) for Stieltjes measures which are used in §18.39(iii); see also Shohat and Tamarkin (1970, Chapter II). Friedman (1990) gives an overview of generalized functions and their relation to distributions. See also Lighthill (1958), and Zemanian (1987).