The Wiener-Hopf method is a powerful technique which enables certain linear partial differential equations subject to boundary conditions on semi-infinite domains to be solved explicitly. The method is sometimes referred to as the Wiener-Hopf technique or the Wiener-Hopf factorization.
The Wiener-Hopf method begins by applying the generalized upper and lower Fourier transforms to obtain an identity
(1)
|
on a strip
(2)
|
of the complex -plane where
is a complex
variable. Note that identity () is in terms of the unknown functions
and
which are analytic
in the half-planes
and
, respectively, while
,
, and
are "parameter functions" in the
-plane which are analytic on all of
.
For simplicity, assume that and
are non-zero in
. The most fundamental step of the Wiener-Hopf process is to
find a solution for
and
in () by finding functions
and
--analytic and nonzero
in
and in
,
respectively--so that
(3)
|
Upon doing so, the factorization () can be used to rewrite () as
(4)
|
whereby the last summand can be decomposed as
(5)
|
for ,
respectively
,
analytic in the region of
satisfying
, respectively
.
Substituting () into () and rewriting induces a function of the form
(6)
|
which, despite being defined only in the strip , can be defined and made analytic on the entire complex
-plane by way of analytic
continuation. The idea behind () is to next show the existence of positive
integers
for which
(7)
|
and
(8)
|
whereby Liouville's theorem applies and requires that
be a polynomial
of degree less
than or equal to
.
In particular,
(9)
|
and
(10)
|
thus defining
and
to within the arbitrary polynomial
, i.e., to within a finite number of arbitrary constants
which must be determined using other methods.
While the Wiener-Hopf method itself is a useful tool for solving various types of partial differential equations, one of its most significant strengths is the vast array of other equation solving methods derived therefrom. Indeed, the techniques spawned from the Wiener-Hopf factorization have proven useful in a number of very different circumstances across a diverse array of disciplines including theoretical and applied physics (Noble 1958), diffraction theory (Linton and McIver 2001), and fluid dynamics (Ho 2007).