Dirichlet space

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In mathematics, the Dirichlet space on the domain Ωβ„‚,π’Ÿ(Ω) (named after Peter Gustav Lejeune Dirichlet), is the reproducing kernel Hilbert space of holomorphic functions, contained within the Hardy space H2(Ω), for which the Dirichlet integral, defined by

π’Ÿ(f):=1πΩ|f(z)|2dA=14πΩ|xf|2+|yf|2dxdy

is finite (here dA denotes the area Lebesgue measure on the complex plane β„‚). The latter is the integral occurring in Dirichlet's principle for harmonic functions. The Dirichlet integral defines a seminorm on π’Ÿ(Ω). It is not a norm in general, since π’Ÿ(f)=0 whenever f is a constant function.

For f,gπ’Ÿ(Ω), we define

π’Ÿ(f,g):=1πΩf(z)g(z)dA(z).

This is a semi-inner product, and clearly π’Ÿ(f,f)=π’Ÿ(f). We may equip π’Ÿ(Ω) with an inner product given by

f,gπ’Ÿ(Ω):=f,gH2(Ω)+π’Ÿ(f,g)(f,gπ’Ÿ(Ω)),

where ,H2(Ω) is the usual inner product on H2(Ω). The corresponding norm π’Ÿ(Ω) is given by

fπ’Ÿ(Ω)2:=fH2(Ω)2+π’Ÿ(f)(fπ’Ÿ(Ω)).

Note that this definition is not unique, another common choice is to take f2=|f(c)|2+π’Ÿ(f), for some fixed cΩ.

The Dirichlet space is not an algebra, but the space π’Ÿ(Ω)H(Ω) is a Banach algebra, with respect to the norm

fπ’Ÿ(Ω)H(Ω):=fH(Ω)+π’Ÿ(f)1/2(fπ’Ÿ(Ω)H(Ω)).


We usually have Ω=𝔻 (the unit disk of the complex plane β„‚), in that case π’Ÿ(𝔻):=π’Ÿ, and if

f(z)=n0anzn(fπ’Ÿ),

then

D(f)=n1n|an|2,

and

fπ’Ÿ2=n0(n+1)|an|2.

Clearly, π’Ÿ contains all the polynomials and, more generally, all functions f, holomorphic on 𝔻 such that f is bounded on 𝔻.

The reproducing kernel of π’Ÿ at wβ„‚{0} is given by

kw(z)=1zwlog(11zw)(zβ„‚{0}).

See also

References

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