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The refined multifractal formalism of some homogeneous Moran measures

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Abstract

The concept of dimension is an important task in geometry. It permits a description of the growth process of objects. It may be seen as an invariant measure characterizing the object. Fractal dimensions are a kind of invariants permitting essentially to describe the irregularity hidden in irregular objects, by providing a suitable growth law. Among fractal geometrical objects, Moran’s types play an important role in explaining many situations, in pure mathematics as the general context of Cantor’s, and in applied physics as a suitable context for studying scaling laws. In the present paper, some non-regular homogeneous Moran measures are investigated, by establishing some new sufficient conditions permitting an explicit computation of the relative multifractal dimensions of the level sets for which the classical formulation does not hold. Besides, the mutual singularity of the relative multifractal measures for the homogeneous Moran case with different multifractal dimensions is investigated. This is very important, as in quasi-all existing situations, the validity of the multifractal formalism passes through the equality of the multifractal Hausdorff dimension with the packing one.

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... Numerous writers have looked at these measures, stressing their significance for the study of local fractal properties and fractal products [2,4,24,25,26,33,43]. In particular, Cole introduced in [14] a generalized Hausdorff and packing measures H q,s µ and P q,s µ respectively (see [1,2,4,6,17,19,34,48,50,51] for more details on these measures and their applications) in order to introduce a general formalism for the multifractal analysis of one probability measure µ with respect to an other measure ν. More specifically, he calculated, for α ≥ 0, the size of the set E(α) = x ∈ supp µ ∩ supp ν; lim r→0 log µ(B(x, r)) log ν(B(x, r)) = α , (1.1) where supp µ is the topological support of the measure µ and B(x, r) stand for the closed ball of center x and radius r. ...
... These are straightforward analogues of the so-called thermodynamic formalism's characterization of the dimensions of repellers. We define now the pressure function Π and the Gibbs measure π q,t (see [19]) respectively by ...
... A simple calculation gives that Given q ∈ R, there exists from [19] a probability measure π q,β(q) supported by E such that for any n ≥ 1 and σ 0 ∈ D n , π q,β(q) (σ 1 σ 2 · · · σ n ) = µ (I σ0 ) q ν (I σ0 ) β(q) σ∈Dn µ (I σ ) q ν (I σ ) β(q) . ...
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