The space of test functions consists of infinitely differentiable real-valued functions whose support of a function is a compact subset of .
Equip with the Dirichlet inner product
The zero-boundary Sobolev space is its Hilbert space completion in the norm .
The zero-boundary Gaussian free field on is the isonormal Gaussian process over : for , the variables are centered jointly Gaussian and satisfy
Equivalently, for an orthonormal basis of and independent standard normal variables ,
as a random generalized function.
For an open subdomain , identify with the closed subspace of obtained by zero extension. Its orthogonal complement is
If , then testing against and integrating by parts gives in in the distributional derivative sense. The Weyl lemma therefore gives a representative harmonic on .
The orthogonal decomposition by a closed subspace gives
Project the isonormal process defining onto these two orthogonal subspaces. The projections are jointly Gaussian and uncorrelated, hence independent. The first projection is a zero-boundary Gaussian free field on ; the second is a random distribution that is harmonic on . Thus
with independent summands. This proves the Domain Markov property of the Gaussian free field.
The zero-Dirichlet Green function of the Laplacian is symmetric, vanishes at the boundary in the appropriate sense, is harmonic in away from , and satisfies
as a distribution. Equivalently, for suitable ,
For , set
and define the distributional pairing by
It is centered Gaussian by the definition of the GFF. Integration by parts gives
This is the Test-function pairing with a Gaussian free field.
Choose an orthonormal basis of and write the GFF formally as , where the are independent standard normal variables. The Green-kernel expansion in the Dirichlet space gives
Consequently the series
converges in . Its partial sums are centered Gaussian and their variances converge to the displayed Green energy. The limit is therefore Gaussian with mean zero and variance
This constructs the Finite-Green-energy measure pairing with a Gaussian free field independently of the chosen orthonormal basis.

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