In mathematics, the Dirichlet space on the domain
(named after Peter Gustav Lejeune Dirichlet), is the reproducing kernel Hilbert space of holomorphic functions, contained within the Hardy space
, for which the Dirichlet integral, defined by

is finite (here dA denotes the area Lebesgue measure on the complex plane
). The latter is the integral occurring in Dirichlet's principle for harmonic functions. The Dirichlet integral defines a seminorm on
. It is not a norm in general, since
whenever f is a constant function.
For
, we define

This is a semi-inner product, and clearly
. We may equip
with an inner product given by

where
is the usual inner product on
The corresponding norm
is given by

Note that this definition is not unique, another common choice is to take
, for some fixed
.
The Dirichlet space is not an algebra, but the space
is a Banach algebra, with respect to the norm

We usually have
(the unit disk of the complex plane
), in that case
, and if

then

and

Clearly,
contains all the polynomials and, more generally, all functions
, holomorphic on
such that
is bounded on
.
The reproducing kernel of
at
is given by
