Dirichlet form

When working on ${\displaystyle \mathbb {R} ^{n}}$, the "classical" Dirichlet form is given by:

${\displaystyle {\mathcal {E}}(u,v)=\int _{\mathbb {R} ^{n}}\nabla u(x)\cdot \nabla v(x)\;dx}$

where one often discusses ${\displaystyle {\mathcal {E}}(u):={\mathcal {E}}(u,u)=\|\nabla u\|_{2}^{2}}$ which is often referred to as the "energy" of the function ${\displaystyle u(x)}$.

More generally, a Dirichlet form is a Markovian closed symmetric form on an L²-space.[1] In particular, A Dirichlet form on a measure space ${\displaystyle (X,\mu )}$ is a bilinear function

${\displaystyle {\mathcal {E}}:D\times D\to \mathbb {R} }$

such that

1) ${\displaystyle D}$ is a dense subset of ${\displaystyle L^{2}(X,\mu )}$

2) ${\displaystyle {\mathcal {E}}}$ is symmetric, that is ${\displaystyle {\mathcal {E}}(u,v)={\mathcal {E}}(v,u)}$ for every ${\displaystyle u,v\in D}$.

3) ${\displaystyle {\mathcal {E}}(u,u)\geq 0}$ for every ${\displaystyle u\in D}$.

4) The set ${\displaystyle D}$ equipped with the inner product defined by ${\displaystyle (u,v)_{\mathcal {E}}:=(u,v)_{L^{2}(X,\mu )}+{\mathcal {E}}(u,v)}$ is a real Hilbert space.

5) For every ${\displaystyle u\in D}$ we have that ${\displaystyle u_{*}=\min(\max(u,0),1)\in D}$ and ${\displaystyle {\mathcal {E}}(u_{*},u_{*})\leq {\mathcal {E}}(u,u)}$

In other words, a Dirichlet form is nothing but a non negative symmetric bilinear form defined on a dense subset of ${\displaystyle L^{2}(X,\mu )}$ such that 4) and 5) hold.

Alternatively, the quadratic form ${\displaystyle u\to {\mathcal {E}}(u,u)}$ itself is known as the Dirichlet form and it is still denoted by ${\displaystyle {\mathcal {E}}}$, so ${\displaystyle {\mathcal {E}}(u):={\mathcal {E}}(u,u)}$.

Functions that minimize the energy given certain boundary conditions are called harmonic, and the associated Laplacian (weak or not) will be zero on the interior, as expected.

For example, let ${\displaystyle {\mathcal {E}}}$ be standard Dirichlet form defined for ${\displaystyle u\in H^{1}(\mathbb {R} ^{n})}$ as

${\displaystyle {\mathcal {E}}(u)=\int _{\mathbb {R} ^{n}}|\nabla u|^{2}\;dx}$

Then a harmonic function in the standard sense, i.e. such that ${\displaystyle \Delta u=0}$, will have ${\displaystyle {\mathcal {E}}(u)=0}$ as can be seen with integration by parts.

As an alternative example, the standard graph Dirichlet form is given by:

${\displaystyle {\mathcal {E}}_{G}(u,v)=\sum _{x\sim y}((u(x)-u(y))(v(x)-v(y))}$

where ${\displaystyle x\sim y}$ means they are connected by an edge. Let a subset of the vertex set be chosen, and call it the boundary of the graph. Assign a Dirichlet boundary condition (choose real numbers for each boundary vertex). One can find a function that minimizes the graph energy, and it will be harmonic. In particular, it will satisfy the averaging property, which is embodied by the graph Laplacian, that is, if ${\displaystyle u_{G}(x)}$ is a graph harmonic then ${\displaystyle \Delta _{G}u_{G}(x)=\sum _{y\sim x}(u_{G}(y)-u_{G}(x))=0}$ which is equivalent to the averaging property ${\displaystyle u_{G}(x)={\frac {1}{|\{y:y\sim x\}|}}\sum _{y\sim x}u_{G}(y)}$ .

Technically, such objects are studied in abstract potential theory, based on the classical Dirichlet's principle. The theory of Dirichlet forms originated in the work of Beurling and Deny (1958, 1959) on Dirichlet spaces.

Another example of a Dirichlet form is given by

${\displaystyle {\mathcal {E}}(u)=\iint _{\mathbb {R} ^{n}\times \mathbb {R} ^{n}}(u(y)-u(x))^{2}k(x,y)\,\mathrm {d} x\,\mathrm {d} y}$

where ${\displaystyle k:\mathbb {R} ^{n}\times \mathbb {R} ^{n}\to \mathbb {R} }$ is some non-negative symmetric integral kernel.

If the kernel ${\displaystyle k}$ satisfies the bound ${\displaystyle k(x,y)\leq \Lambda |x-y|^{-n-s}}$, then the quadratic form is bounded in ${\displaystyle {\dot {H}}^{s/2}}$. If moreover, ${\displaystyle \lambda |x-y|^{-n-s}\leq k(x,y)}$, then the form is comparable to the norm in ${\displaystyle {\dot {H}}^{s/2}}$ squared and in that case the set ${\displaystyle D\subset L^{2}(\mathbb {R} ^{n})}$ defined above is given by ${\displaystyle H^{s/2}(\mathbb {R} ^{n})}$. Thus Dirichlet forms are natural generalizations of the Dirichlet integrals

${\displaystyle {\mathcal {E}}(u)=\int (A\nabla u,\nabla u)\;\mathrm {d} x,}$

where ${\displaystyle A(x)}$ is a positive symmetric matrix. The Euler-Lagrange equation of a Dirichlet form is a non-local analogue of an elliptic equations in divergence form. Equations of this type are studied using variational methods and they are expected to satisfy similar properties.[2][3][4]

• Beurling, Arne; Deny, J. (1958), "Espaces de Dirichlet. I. Le cas élémentaire", Acta Mathematica, 99 (1): 203–224, doi:10.1007/BF02392426, ISSN 0001-5962, MR 0098924
• Beurling, Arne; Deny, J. (1959), "Dirichlet spaces", Proceedings of the National Academy of Sciences of the United States of America, 45 (2): 208–215, Bibcode:1959PNAS...45..208B, doi:10.1073/pnas.45.2.208, ISSN 0027-8424, JSTOR 90170, MR 0106365, PMC 222537, PMID 16590372
• Fukushima, Masatoshi (1980), Dirichlet forms and Markov processes, North-Holland Mathematical Library, 23, Amsterdam: North-Holland, ISBN 978-0-444-85421-6, MR 0569058
• Jost, Jürgen; Kendall, Wilfrid; Mosco, Umberto; Röckner, Michael; Sturm, Karl-Theodor (1998), New directions in Dirichlet forms, AMS/IP Studies in Advanced Mathematics, 8, Providence, RI: American Mathematical Society, p. xiv+277, ISBN 978-0-8218-1061-3, MR 1652277.
• "Abstract potential theory", Encyclopedia of Mathematics, EMS Press, 2001 [1994]