Bessel Potential
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mathematics Mathematics is an area of knowledge that includes the topics of numbers, formulas and related structures, shapes and the spaces in which they are contained, and quantities and their changes. These topics are represented in modern mathematics ...
, the Bessel potential is a
potential Potential generally refers to a currently unrealized ability. The term is used in a wide variety of fields, from physics to the social sciences to indicate things that are in a state where they are able to change in ways ranging from the simple re ...
(named after
Friedrich Wilhelm Bessel Friedrich Wilhelm Bessel (; 22 July 1784 – 17 March 1846) was a German astronomer, mathematician, physicist, and geodesist. He was the first astronomer who determined reliable values for the distance from the sun to another star by the method ...
) similar to the
Riesz potential In mathematics, the Riesz potential is a potential named after its discoverer, the Hungarian mathematician Marcel Riesz. In a sense, the Riesz potential defines an inverse for a power of the Laplace operator on Euclidean space. They generalize to ...
but with better decay properties at infinity. If ''s'' is a complex number with positive real part then the Bessel potential of order ''s'' is the operator :(I-\Delta)^ where Δ is the
Laplace operator In mathematics, the Laplace operator or Laplacian is a differential operator given by the divergence of the gradient of a scalar function on Euclidean space. It is usually denoted by the symbols \nabla\cdot\nabla, \nabla^2 (where \nabla is the ...
and the fractional power is defined using Fourier transforms.
Yukawa potential In particle, atomic and condensed matter physics, a Yukawa potential (also called a screened Coulomb potential) is a potential named after the Japanese physicist Hideki Yukawa. The potential is of the form: :V_\text(r)= -g^2\frac, where is a m ...
s are particular cases of Bessel potentials for s=2 in the 3-dimensional space.


Representation in Fourier space

The Bessel potential acts by multiplication on the
Fourier transform A Fourier transform (FT) is a mathematical transform that decomposes functions into frequency components, which are represented by the output of the transform as a function of frequency. Most commonly functions of time or space are transformed, ...
s: for each \xi \in \mathbb^d : \mathcal((I-\Delta)^ u) (\xi)= \frac.


Integral representations

When s > 0, the Bessel potential on \mathbb^d can be represented by :(I - \Delta)^ u = G_s \ast u, where the Bessel kernel G_s is defined for x \in \mathbb^d \setminus \ by the integral formula : G_s (x) = \frac \int_0^\infty \frac\,\mathrmy. Here \Gamma denotes the
Gamma function In mathematics, the gamma function (represented by , the capital letter gamma from the Greek alphabet) is one commonly used extension of the factorial function to complex numbers. The gamma function is defined for all complex numbers except ...
. The Bessel kernel can also be represented for x \in \mathbb^d \setminus \ by : G_s (x) = \frac \int_0^\infty e^ \Big(t + \frac\Big)^\frac \,\mathrmt. This last expression can be more succinctly written in terms of a modified
Bessel function Bessel functions, first defined by the mathematician Daniel Bernoulli and then generalized by Friedrich Bessel, are canonical solutions of Bessel's differential equation x^2 \frac + x \frac + \left(x^2 - \alpha^2 \right)y = 0 for an arbitrary ...
, for which the potential gets its name: : G_s(x)=\fracK_(\vert x \vert) \vert x \vert^.


Asymptotics

At the origin, one has as \vert x\vert \to 0 , : G_s (x) = \frac(1 + o (1)) \quad \text 0 < s < d, : G_d (x) = \frac\ln \frac(1 + o (1)) , : G_s (x) = \frac(1 + o (1)) \quad \texts > d. In particular, when 0 < s < d the Bessel potential behaves asymptotically as the
Riesz potential In mathematics, the Riesz potential is a potential named after its discoverer, the Hungarian mathematician Marcel Riesz. In a sense, the Riesz potential defines an inverse for a power of the Laplace operator on Euclidean space. They generalize to ...
. At infinity, one has, as \vert x\vert \to \infty , : G_s (x) = \frac(1 + o (1)).


See also

*
Riesz potential In mathematics, the Riesz potential is a potential named after its discoverer, the Hungarian mathematician Marcel Riesz. In a sense, the Riesz potential defines an inverse for a power of the Laplace operator on Euclidean space. They generalize to ...
*
Fractional integration In fractional calculus, an area of mathematical analysis, the differintegral (sometime also called the derivigral) is a combined differentiation/ integration operator. Applied to a function ƒ, the ''q''-differintegral of ''f'', here denoted ...
*
Sobolev space In mathematics, a Sobolev space is a vector space of functions equipped with a norm that is a combination of ''Lp''-norms of the function together with its derivatives up to a given order. The derivatives are understood in a suitable weak sense t ...
*
Fractional Schrödinger equation A fraction is one or more equal parts of something. Fraction may also refer to: * Fraction (chemistry), a quantity of a substance collected by fractionation * Fraction (floating point number), an (ambiguous) term sometimes used to specify a part ...
*
Yukawa potential In particle, atomic and condensed matter physics, a Yukawa potential (also called a screened Coulomb potential) is a potential named after the Japanese physicist Hideki Yukawa. The potential is of the form: :V_\text(r)= -g^2\frac, where is a m ...


References

* * * * * {{citation , first=Elias , last=Stein , authorlink=Elias Stein , title=Singular integrals and differentiability properties of functions , publisher=
Princeton University Press Princeton University Press is an independent publisher with close connections to Princeton University. Its mission is to disseminate scholarship within academia and society at large. The press was founded by Whitney Darrow, with the financial su ...
, location=Princeton, NJ , year=1970 , isbn=0-691-08079-8 , url-access=registration , url=https://archive.org/details/singularintegral0000stei Fractional calculus Partial differential equations Potential theory Singular integrals