In mathematics, and specifically in potential theory, the Poisson kernel is an integral kernel, used for solving the two-dimensional Laplace equation, given Dirichlet boundary conditions on the unit disk.
The kernel can be understood as the derivative of the Green's function for the Laplace equation.
Poisson kernels commonly find applications in control theory and two-dimensional problems in electrostatics.
In practice, the definition of Poisson kernels are often extended to n-dimensional problems.
In the complex plane, the Poisson kernel for the unit disc [1] is given by
is harmonic in D and has a radial limit that agrees with f almost everywhere on the boundary T of the disc.
That the boundary value of u is f can be argued using the fact that as r → 1, the functions Pr(θ) form an approximate unit in the convolution algebra L1(T).
As linear operators, they tend to the Dirac delta function pointwise on Lp(T).
By the maximum principle, u is the only such harmonic function on D. Convolutions with this approximate unit gives an example of a summability kernel for the Fourier series of a function in L1(T) (Katznelson 1976).
After the Fourier transform, convolution with Pr(θ) becomes multiplication by the sequence {r|k|} ∈ ℓ1(Z).
[further explanation needed] Taking the inverse Fourier transform of the resulting product {r|k|fk} gives the Abel means Arf of f:
Rearranging this absolutely convergent series shows that f is the boundary value of g + h, where g (resp.
antiholomorphic) function on D. When one also asks for the harmonic extension to be holomorphic, then the solutions are elements of a Hardy space.
This is true when the negative Fourier coefficients of f all vanish.
In particular, the Poisson kernel is commonly used to demonstrate the equivalence of the Hardy spaces on the unit disk, and the unit circle.
Since Lp(T) is a Banach space (for 1 ≤ p ≤ ∞), so is Hp(T).
The unit disk may be conformally mapped to the upper half-plane by means of certain Möbius transformations.
Since the conformal map of a harmonic function is also harmonic, the Poisson kernel carries over to the upper half-plane.
In this case, the Poisson integral equation takes the form
, the Lp space of integrable functions on the real line, u can be understood as a harmonic extension of f into the upper half-plane.
In analogy to the situation for the disk, when u is holomorphic in the upper half-plane, then u is an element of the Hardy space,
Thus, again, the Hardy space Hp on the upper half-plane is a Banach space, and, in particular, its restriction to the real axis is a closed subspace of
The situation is only analogous to the case for the unit disk; the Lebesgue measure for the unit circle is finite, whereas that for the real line is not.
the Poisson kernel takes the form
An expression for the Poisson kernel of an upper half-space can also be obtained.
Denote the standard Cartesian coordinates of
The upper half-space is the set defined by
The Poisson kernel for the upper half-space appears naturally as the Fourier transform of the Abel transform in which t assumes the role of an auxiliary parameter.
In particular, it is clear from the properties of the Fourier transform that, at least formally, the convolution
is a solution of Laplace's equation in the upper half-plane.