Weyl's Lemma (Laplace Equation)
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In
mathematics Mathematics is a field of study that discovers and organizes methods, Mathematical theory, theories and theorems that are developed and Mathematical proof, proved for the needs of empirical sciences and mathematics itself. There are many ar ...
, Weyl's lemma, named after
Hermann Weyl Hermann Klaus Hugo Weyl (; ; 9 November 1885 – 8 December 1955) was a German mathematician, theoretical physicist, logician and philosopher. Although much of his working life was spent in Zürich, Switzerland, and then Princeton, New Jersey, ...
, states that every weak solution of
Laplace's equation In mathematics and physics, Laplace's equation is a second-order partial differential equation named after Pierre-Simon Laplace, who first studied its properties in 1786. This is often written as \nabla^2\! f = 0 or \Delta f = 0, where \Delt ...
is a smooth solution. This contrasts with the
wave equation The wave equation is a second-order linear partial differential equation for the description of waves or standing wave fields such as mechanical waves (e.g. water waves, sound waves and seismic waves) or electromagnetic waves (including light ...
, for example, which has weak solutions that are not smooth solutions. Weyl's lemma is a special case of elliptic or hypoelliptic regularity.


Statement of the lemma

Let \Omega be an
open subset In mathematics, an open set is a generalization of an open interval in the real line. In a metric space (a set with a distance defined between every two points), an open set is a set that, with every point in it, contains all points of the met ...
of n-dimensional Euclidean space \mathbb^, and let \Delta denote the usual
Laplace operator In mathematics, the Laplace operator or Laplacian is a differential operator given by the divergence of the gradient of a Scalar field, scalar function on Euclidean space. It is usually denoted by the symbols \nabla\cdot\nabla, \nabla^2 (where \ ...
. Weyl's lemma states that if a
locally integrable In mathematics, a locally integrable function (sometimes also called locally summable function) is a function which is integrable (so its integral is finite) on every compact subset of its domain of definition. The importance of such functions li ...
function u \in L_^(\Omega) is a weak solution of Laplace's equation, in the sense that :\int_\Omega u(x) \, \Delta \varphi (x) \, dx = 0 for every
test function In mathematical analysis, a bump function (also called a test function) is a function f : \Reals^n \to \Reals on a Euclidean space \Reals^n which is both smooth (in the sense of having continuous derivatives of all orders) and compactly suppor ...
( smooth function with
compact support In mathematics, the support of a real-valued function f is the subset of the function domain of elements that are not mapped to zero. If the domain of f is a topological space, then the support of f is instead defined as the smallest closed ...
) \varphi \in C_c^\infty(\Omega), then (up to redefinition on a set of
measure zero In mathematical analysis, a null set is a Lebesgue measurable set of real numbers that has Lebesgue measure, measure zero. This can be characterized as a set that can be Cover (topology), covered by a countable union of Interval (mathematics), ...
) u \in C^(\Omega) is smooth and satisfies \Delta u = 0 pointwise in \Omega. This result implies the interior regularity of
harmonic function In mathematics, mathematical physics and the theory of stochastic processes, a harmonic function is a twice continuously differentiable function f\colon U \to \mathbb R, where is an open subset of that satisfies Laplace's equation, that i ...
s in \Omega, but it does not say anything about their regularity on the boundary \partial\Omega.


Idea of the proof

To prove Weyl's lemma, one convolves the function u with an appropriate mollifier \varphi_\varepsilon and shows that the mollification u_\varepsilon = \varphi_\varepsilon\ast u satisfies Laplace's equation, which implies that u_\varepsilon has the mean value property. Taking the limit as \varepsilon\to 0 and using the properties of mollifiers, one finds that u also has the mean value property, which implies that it is a smooth solution of Laplace's equation. Alternative proofs use the smoothness of the fundamental solution of the Laplacian or suitable a priori elliptic estimates.


Generalization to distributions

More generally, the same result holds for every distributional solution of Laplace's equation: If T\in D'(\Omega) satisfies \langle T, \Delta \varphi\rangle = 0 for every \varphi\in C_c^\infty(\Omega), then T is a regular distribution associated with a smooth solution u\in C^\infty(\Omega) of Laplace's equation.


Connection with hypoellipticity

Weyl's lemma follows from more general results concerning the regularity properties of elliptic or hypoelliptic operators. Lars Hörmander, ''The Analysis of Linear Partial Differential Operators I'', 2nd ed., Springer-Verlag (1990), p.110 A linear partial differential operator P with smooth coefficients is hypoelliptic if the singular support of P u is equal to the singular support of u for every distribution u. The Laplace operator is hypoelliptic, so if \Delta u = 0, then the singular support of u is empty since the singular support of 0 is empty, meaning that u\in C^\infty(\Omega). In fact, since the Laplacian is elliptic, a stronger result is true, and solutions of \Delta u = 0 are real-analytic.


Notes


References

* *{{cite book , first=Elias , last=Stein , authorlink=Elias Stein, year=2005 , title=Real Analysis: Measure Theory, Integration, and Hilbert Spaces , publisher=Princeton University Press , isbn=0-691-11386-6 Lemmas in mathematical analysis Partial differential equations Harmonic functions