1996
DOI: 10.1007/bf03167295
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On eigenvalue problems for Laplacians on P.C.F. self-similar sets

Abstract: We formulate and study a strong harmonic structure under which eigenvalues of the Laplacian on a p.c.f, self-similar set are completely determined according to the dynamical system generated by a rational function. We then show that, with some additional assumptions, the eigenvalue counting function p(A) behaves so wildly that p()~) does not vary regularly, and the ratio p(~)/)t ds/2 is bounded but non-convergent as A q cr where ds is the spectral dimension of the p.c.f, self-similar set.

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Cited by 78 publications
(88 citation statements)
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“…There are, of course, many more examples in which the number of terminal points is finite, such as the Sierpinski gaskets based on higher dimensional simplices. One would also want the spectral decimation method of [Sh2] or [MT] to hold.…”
Section: Fractafolds Based On the Sierpinski Gasket 4021mentioning
confidence: 99%
See 1 more Smart Citation
“…There are, of course, many more examples in which the number of terminal points is finite, such as the Sierpinski gaskets based on higher dimensional simplices. One would also want the spectral decimation method of [Sh2] or [MT] to hold.…”
Section: Fractafolds Based On the Sierpinski Gasket 4021mentioning
confidence: 99%
“…In fact, the matching conditions provide necessary and sufficient conditions for gluing together local solutions ∆u i = f i on C i to obtain a global solution ∆u = f (here we assume that the glued functions u and f are continuous). The spectrum of the Laplacian on SG (with Dirichlet or Neumann boundary conditions) was described exactly by Fukushima and Shima [FS], [Sh1] (see also [DSV], [MT], [T] and [GRS] for further elaborations) based on the method of spectral decimation [Sh2]. Our goal is to give an analogous description for fractafolds.…”
Section: Spectrum Of the Laplacianmentioning
confidence: 99%
“…Then −∆ on dom L 2 ∆ becomes a positive selfadjoint operator under Dirichlet boundary conditions with compact inverse (or under Neumann boundary conditions with compact resolvant), and so has a discrete spectrum, with eigenfunctions belonging to domD. In fact the nature of the eigenvalues and eigenfunctions is known explicity via the method of spectral decimation of Fukushima and Shima ([4], [15], [16]). For functions in domD there is also a pointwise formula for ∆u as a limit of a difference quotient…”
Section: E(u)mentioning
confidence: 99%
“…The Laplacian on the Vicsek set has been studied extensively in [Barlow 1998;Malozemov and Teplyaev 2003;Metz 1993;Shima 1996], both analytically and probabilistically. Various problems have been studied for this fractal, including topological rigidity [Strichartz 2006], the uniqueness of Brownian motion [Metz 1993], etc.…”
Section: Introductionmentioning
confidence: 99%
“…In this paper, we study the spectrum of the Laplacian on a special case of this infinite family of fractals, the symmetric n-branch Vicsek set ᐂ n . All eigenvalues of the Laplacian can be obtained through an iterative process called spectral decimation, which was introduced by Shima [1996]. It turns out that the spectral decimation function is associated with the Chebyshev polynomials.…”
Section: Introductionmentioning
confidence: 99%