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Journal of the London Mathematical Society 2004 69(3):657-675; doi:10.1112/S002461070300512X
© 2004 by London Mathematical Society
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© The London Mathematical Society

Eigenvalues of the Radially Symmetric p-Laplacian in Rn

B. M. Brown and W. Reichel

Department of Computer Science, University of Cardiff Cardiff CF2 3XF, United Kingdom
Mathematisches Institut, Universität Basel Rheinsprung 21, CH-4051 Basel, Switzerland

Received 2 June 2003.

For the p-Laplacian {Delta}p{upsilon} = div:(| {nabla}{upsilon}|p–2{nabla}{upsilon}), p>1, the eigenvalue problem –{Delta}p{upsilon} + q(|x|)|{upsilon}|p–2{upsilon} = {lambda}|{upsilon}|p–2{upsilon} in Rn is considered under the assumption of radial symmetry. For a first class of potentials q(r)->{infty} as r->{infty} at a sufficiently fast rate, the existence of a sequence of eigenvalues {lambda}k->{infty} if k->{infty} is shown with eigenfunctions belonging to Lp(Rn). In the case p=2, this corresponds to Weyl's limit point theory. For a second class of power-like potentials q(r)->{infty} as r->{infty} at a sufficiently fast rate, it is shown that, under an additional boundary condition at r={infty}, which generalizes the Lagrange bracket, there exists a doubly infinite sequence of eigenvalues {lambda}k with {lambda}k -> ±{infty} if k->±{infty}. In this case, every solution of the initial value problem belongs to Lp(Rn). For p=2, this situation corresponds to Weyl's limit circle theory.


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