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Multifractal measures,especially for the geophysicist
Authors:Benoît B. Mandelbrot
Affiliation:(1) Physics Department, IBM T. J. Watson Research Center, 10598 Yorktown Heights, NY, USA;(2) Mathematics Department, Yale University, 06520 New Haven, CT, USA
Abstract:This text is addressed to both the beginner and the seasoned professional, geology being used as the main but not the sole illustration. The goal is to present an alternative approach to multifractals, extending and streamlining the original approach inMandelbrot (1974). The generalization from fractalsets to multifractalmeasures involves the passage from geometric objects that are characterized primarily by one number, namely a fractal dimension, to geometric objects that are characterized primarily by a function. The best is to choose the function rhov(agr), which is a limit probability distribution that has been plotted suitably, on double logarithmic scales. The quantity agr is called Hölder exponent. In terms of the alternative functionf(agr) used in the approach of Frisch-Parisi and of Halseyet al., one has rhov(agr)=f(agr)–E for measures supported by the Euclidean space of dimensionE. Whenf(agr)ge0,f(agr) is a fractal dimension. However, one may havef(agr)<0, in which case agr is called ldquolatent.rdquo One may even have agr<0, in which case agr is called ldquovirtual.rdquo These anomalies' implications are explored, and experiments are suggested. Of central concern in this paper is the study of low-dimensional cuts through high-dimensional multifractals. This introduces a quantityDq, which is shown forq>1 to be a critical dimension for the cuts. An ldquoenhanced multifractal diagramrdquo is drawn, includingf(agr), a function called tau(q) andDq.This text incorporatesand supersedesMandelbrot (1988). A more detailed treatment, in preparation, will incorporateMandelbrot (1989).
Keywords:Fractal  multifractal  measure    lder  limit theorem
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