Weyl law

  (Redirected from Weyl's law)

In mathematics, especially spectral theory, Weyl's law describes the asymptotic behavior of eigenvalues of the Laplace–Beltrami operator. This description was discovered in 1911 (in the case) by Hermann Weyl for eigenvalues for the Laplace–Beltrami operator acting on functions that vanish at the boundary of a bounded domain . In particular, he proved that the number, , of Dirichlet eigenvalues (counting their multiplicities) less than or equal to satisfies

where is a volume of the unit ball in .[1] In 1912 he provided a new proof based on variational methods.[2][3]

GeneralizationsEdit

The Weyl law has been extended to more general domains and operators. For the Schrödinger operator

 

it was extended to

 

as   tending to   or to a bottom of essential spectrum and/or  .

Here   is the number of eigenvalues of   below   unless there is essential spectrum below   in which case  .

In the development of spectral asymptotics, the crucial role was played by variational methods and microlocal analysis.

Counter-examplesEdit

The extended Weyl law fails in certain situations. In particular, the extended Weyl law "claims" that there is no essential spectrum if and only if the right-hand expression is finite for all  .

If one considers domains with cusps (i.e. "shrinking exits to infinity") then the (extended) Weyl law claims that there is no essential spectrum if and only if the volume is finite. However for the Dirichlet Laplacian there is no essential spectrum even if the volume is infinite as long as cusps shrinks at infinity (so the finiteness of the volume is not necessary).

On the other hand, for the Neumann Laplacian there is an essential spectrum unless cusps shrinks at infinity faster than the negative exponent (so the finiteness of the volume is not sufficient).

Weyl conjectureEdit

Weyl conjectured that

 

where the remainder term is negative for Dirichlet boundary conditions and positive for Neumann. The remainder estimate was improved upon by many mathematicians.

In 1922, Richard Courant proved a bound of  . In 1952, Boris Levitan proved the tighter bound of   for compact closed manifolds. Robert Seeley extended this to include certain Euclidean domains in 1978.[4] In 1975, Hans Duistermaat and Victor Guillemin proved the bound of   when the set of periodic bicharacteristics has measure 0.[5] This was finally generalized by Victor Ivrii in 1980.[6] This generalization assumes that the set of periodic trajectories of a billiard in   has measure 0, which Ivrii conjectured is fulfilled for all bounded Euclidean domains with smooth boundaries. Since then, similar results have been obtained for wider classes of operators.

ReferencesEdit

  1. ^ Weyl, Hermann (1911). "Über die asymptotische Verteilung der Eigenwerte". Nachrichten der Königlichen Gesellschaft der Wissenschaften zu Göttingen: 110–117.
  2. ^ "Das asymptotische Verteilungsgesetz linearen partiellen Differentialgleichungen". Math. Ann. 71: 441–479. 1912.
  3. ^ For a proof in English, see Strauss, Walter A. (2008). Partial Differential Equations. John Wiley & Sons. See chapter 11.
  4. ^ A sharp asymptotic estimate for the eigenvalues of the Laplacian in a domain of  . Advances in Mathematics, 102(3):244–264 (1978).
  5. ^ The spectrum of positive elliptic operators and periodic bicharacteristics. Invent. Math. , 29(1):37–79 (1975).
  6. ^ Second term of the spectral asymptotic expansion for the Laplace–Beltrami operator on manifold with boundary. Funct. Anal. Appl. 14(2):98–106 (1980).