2007
DOI: 10.1090/s0002-9939-07-09008-9
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Asymptotics of eigenvalue clusters for Schrödinger operators on the Sierpiński gasket

Abstract: Abstract. In this note we investigate the asymptotic behavior of spectra of Schrödinger operators with continuous potential on the Sierpiński gasket SG. In particular, using the existence of localized eigenfunctions for the Laplacian on SG we show that the eigenvalues of the Schrödinger operator break into clusters around certain eigenvalues of the Laplacian. Moreover, we prove that the characteristic measure of these clusters converges to a measure. Results similar to ours were first observed by A. Weinstein … Show more

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Cited by 10 publications
(5 citation statements)
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“…We also present graphical data from numerical approximations of lower portions of the spectra. Similar results for the spectrum of Schrödinger operators −∆ + V are given in [14].…”
Section: E(u)supporting
confidence: 77%
“…We also present graphical data from numerical approximations of lower portions of the spectra. Similar results for the spectrum of Schrödinger operators −∆ + V are given in [14].…”
Section: E(u)supporting
confidence: 77%
“…Our work is part of a long term study of mathematical physics on fractals and graphs, more specifically, quantum Hall systems with AMO and their topological quantum phases [1][2][3][4][5][6]8,28,35,[48][49][50], in which novel features of physical systems can be associated with the unusual spectral and geometric properties of fractals and graphs compared to smooth manifolds.…”
Section: Introductionmentioning
confidence: 99%
“…Remark 2. Observe that in comparison with (14), the error in ( 19) is decaying at a slower rate. This is a consequence of the fact that, at the optimal N, the eigenfunctions that are not localized at scale N make up a larger proportion (in terms of dimension) of the space E Λ than they do in the spaces E λ with λ ≈ Λ.…”
Section: General Szegö Theorem On Sgmentioning
confidence: 99%
“…For a fixed large j we may then choose N such that the bound in (17) is minimized, which occurs when ǫ ≈ 3 N −j . Setting (3/5) N α = 3 N −j we compute 3 N −j = 3 −jα log(5/3) log 3+α log (5/3) and substitute into (17) to obtain (14), using d j ≈ 3 j . Remark 1.…”
Section: Szegö Limit Theorem On Sg For a Single Eigenspacementioning
confidence: 99%