1993
DOI: 10.2307/2154402
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Harmonic Calculus on P.C.F. Self-Similar Sets

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Cited by 194 publications
(256 citation statements)
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“…For i ∈ S, define a shift operator σ i : → by σ i (ω 1 ω 2 · · · ) = iω 1 ω 2 · · · . Let us suppose that there exists a continuous surjective map π : → K such that ψ i • π = π • σ i for each i ∈ S. We call (K, S, {ψ i } i∈S ) a self-similar structure, following Kigami [15].…”
Section: Frameworkmentioning
confidence: 99%
“…For i ∈ S, define a shift operator σ i : → by σ i (ω 1 ω 2 · · · ) = iω 1 ω 2 · · · . Let us suppose that there exists a continuous surjective map π : → K such that ψ i • π = π • σ i for each i ∈ S. We call (K, S, {ψ i } i∈S ) a self-similar structure, following Kigami [15].…”
Section: Frameworkmentioning
confidence: 99%
“…fractals [11,12] and the spectral decimation method to analyze their spectra developed by Shima [16].…”
Section: Laplacians On Fractals and Spectral Decimation Methodsmentioning
confidence: 99%
“…The (normalized) Laplacian on K can be defined as a limit of the normalized discrete Laplacians m [11] and [12].…”
Section: Laplacians On Fractals and Spectral Decimationmentioning
confidence: 99%
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“…We only remark that if r --1/2, that is, #~ is the Lebesgue measure, then Sn(x) = r We also note that the above system (3), in a sense, corresponds to Poisson equations with boundary conditions and plays an important role in harmonic analysis on fractal sets. See Kigami [6], [7], and Yamaguti, Hata and Kigami…”
mentioning
confidence: 99%