Christoph Bandt- Analysis on the octagasket

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  • 8/3/2019 Christoph Bandt- Analysis on the octagasket

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    Analysis on the octagasket

    Warsaw, 5 December 2007

    Christoph Bandt

    Mathematics, University of Greifswald

    [email protected]

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    Overview

    1. Motivation

    2. Fractals of finite type

    3. Fractal n-gons

    4. Analysis on finitely ramified fractals

    5. Resistance scaling on new spaces

    6. Harmonic structure on octagasket

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    1.1 Fractal analysis

    Classical analysis on fractal spaces.

    Started with Alexander+Orbach and

    Rammal+Toulouse, J. Physique 1982/83

    Many names: Kusuoka, Lindstrom, Barlow,Fukushima, Kigami, Sabot, Kumagai ...

    Various approaches:

    Laplace operator, Dirichlet forms

    Brownian motion Besov spaces harmonic functions resistance metric

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    1.2 Main problem of fractal analysis

    Well-developed theory, diverse methods.

    But: very few examples,all looking like Sierpinski gasket.

    A single point will disconnect the space,

    at least locally.

    Exception: existence of a Brownian motion

    on Sierpinski carpets, proved by Barlow+Bass1990-99 (uniqueness, parameters, self-similarityremain open)We start analysis on a new class of spaces.(still under construction)

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    1.3 Why self-similar sets?

    Take harmonic functions: they can be defined

    in any metric space by the mean-value prop-

    erty:

    f(x) =1

    (S)

    Sf(y) d (y)

    where S is a small sphere around x and is the

    surface measure.

    This makes sense if

    there are many balls or ball-like sets with

    similar structure (symmetry condition)

    there is a concept of surface measure.

    Both conditions hold on appropriate self-similar

    sets: they form a good testbed for analysis.

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    2.1 Self-similar sets

    Mathematically tractable class of fractals

    f1,...,fn contracting similitudes on Rn.

    On C, fk

    (z

    ) =kz

    +ck

    withrk

    =|k|