## Abstract By now the multifractal structure of selfβsimilar measures satisfying the soβcalled Open Set Condition is well understood. However, if the Open Set Condition is not satisfied, then almost nothing is known. In this paper we prove a nontrivial lower bound for the symbolic multifractal spe
The Multifractal Spectrum of Quasi Self-Similar Measures
β Scribed by Toby C O'Neil
- Publisher
- Elsevier Science
- Year
- 1997
- Tongue
- English
- Weight
- 305 KB
- Volume
- 211
- Category
- Article
- ISSN
- 0022-247X
No coin nor oath required. For personal study only.
β¦ Synopsis
We define the notion of quasi self-similar measures and show that for such measures their generalised Hausdorff and packing measures are positive and finite at the critical exponent. In practice this allows easy calculation of their dimension functions. We then show that a coarse form of the multifractal formalism automatically holds for quasi self-similar measures. Examples of quasi self-similar measures include many of the standard constructions of multifractal measures satisfying a strong separation condition, in particular, self-similar measures.
π SIMILAR VOLUMES
We shall show that the oscillations observed by R. S. Strichartz in the Fourier transforms of self-similar measures have a large-scale renormalisation given by a Riesz measure. Vice versa the Riesz measure itself will be shown to be self-similar around every triadic point.
Let K and Β΅ be the self-similar set and the self-similar measure associated with an iterated function system with probabilities (Si, pi)i=1,...,N satisfying the Open Set Condition. Let Ξ£ = {1, . . . , N} N denote the full shift space and let Ο : Ξ£ β K denote the natural projection. The (symbolic) lo
## Abstract In this paper we study the limit behavior of weighted averages of some random sequence related to Bernoulli random variables, and apply the results to average density of selfβsimilar measures. Β© 2011 WILEYβVCH Verlag GmbH & Co. KGaA, Weinheim
The multifractal structure of measures generated by iterated function systems (IFS) with overlaps is, to a large extend, unknown. In this paper we study the local dimension of the m-time convolution of the standard Cantor measure Β΅. By using some combinatoric techniques, we show that the set E of at
Given a n = n square divided into n smaller squares i.e., a n = n . chessboard , how many k = k squares does it contain, where 1 The answer itself turns out to be a square, namely, n q 1 y k . Thus, the total number of squares contained in the n = n square is the sum of the squares: 1 2 q 2 2 q ΠΈΠΈΠΈ