http://dx.doi.org/10.4153/CJM-2008-022-3
Canad. J. Math. 60(2008), 457-480
Published:2008-04-01 Printed: Apr 2008
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Abstract
We define sets with finitely ramified cell structure, which are
generalizations of post-crit8cally finite self-similar
sets introduced by Kigami and of fractafolds introduced by Strichartz. In general,
we do not assume even local self-similarity, and allow countably many cells
connected at each junction point.
In particular, we consider post-critically infinite fractals.
We prove that if Kigami's resistance form
satisfies certain assumptions, then there exists a weak Riemannian metric
such that the energy can be expressed as the integral of the norm squared
of a weak gradient with respect to an energy measure.
Furthermore, we prove that if such a set can be homeomorphically represented
in harmonic coordinates, then for smooth functions the weak gradient can be
replaced by the usual gradient.
We also prove a simple formula for the energy measure Laplacian in harmonic
coordinates.
| Keywords: |
fractals, self-similarity, energy, resistance, Dirichlet forms, diffusions, quantum graphs, generalized Riemannian metric
fractals, self-similarity, energy, resistance, Dirichlet forms, diffusions, quantum graphs, generalized Riemannian metric
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| MSC Classifications: |
28A80, 31C25, 53B99, 58J65, 60J60, 60G18 show english descriptions
Fractals [See also 37Fxx] Dirichlet spaces None of the above, but in this section Diffusion processes and stochastic analysis on manifolds [See also 35R60, 60H10, 60J60] Diffusion processes [See also 58J65] Self-similar processes
28A80 - Fractals [See also 37Fxx] 31C25 - Dirichlet spaces 53B99 - None of the above, but in this section 58J65 - Diffusion processes and stochastic analysis on manifolds [See also 35R60, 60H10, 60J60] 60J60 - Diffusion processes [See also 58J65] 60G18 - Self-similar processes
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© Canadian Mathematical Society, 2013
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