1992
DOI: 10.1112/plms/s3-65.3.604
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Multifractal Decompositions of Digraph Recursive Fractals

Abstract: We prove that the multifractal decomposition behaves as expected for a family of sets K known as digraph recursive fractals, using measures μ of Markov type. For each value of a parameter α between a minimum αmin and maximum αmax, we define ‘multifractal components’ K(α) of K, and show that they are fractals in the sense of Taylor. The dimension f(α) of K(α) is computed from the data of the problem. The typical concave ‘multifractal f(α)’ dimension spectrum curve results. Under appropriate disjointness conditi… Show more

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Cited by 115 publications
(71 citation statements)
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“…As with self-similar sets, the IFSP approach to measures has been extended to socalled graph-directed constructions, to families of random contractive similarities and to families of non-linear contractions; see [1], [9], [17], [53], [55] for further references.…”
Section: Self-similar Setsmentioning
confidence: 99%
“…As with self-similar sets, the IFSP approach to measures has been extended to socalled graph-directed constructions, to families of random contractive similarities and to families of non-linear contractions; see [1], [9], [17], [53], [55] for further references.…”
Section: Self-similar Setsmentioning
confidence: 99%
“…A Moran fractal is a Cantor-type set defined by iteration; it has a tractable structure and has been used extensively for estimating entropies and dimensions (see e.g. [1,11,17,18,21,22]). In our context, we will make use of a special dynamically defined (by the Bowen metric) Moran fractal (Definition 4.1).…”
Section: Spectrum Of Poincaré Recurrence 1919mentioning
confidence: 99%
“…V(i, j) E [l; d + l]*, 3n > 0 [{A(P, Y)}"]i,j > O-this represents the number of cylinders of (e,, starting at i and finishing at j). The largest zero of a polynomial is an analytic function of the coefficients in the region where it is a simple zero [19,Prop. 3:1], and this assures (by the Perron-Frobenius theory of nonnegative matrices) the existence and the uniqueness of the real y1 for which A(& y) has spectral radius equal to 1: we then get y1 = -F(P); fo r example, when /3 = 0, we have y1 = -F(O) = dr.…”
Section: Thermodynamicsmentioning
confidence: 99%