2008
DOI: 10.1103/physreve.77.066203
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Dimensions, maximal growth sites, and optimization in the dielectric breakdown model

Abstract: We study the growth of fractal clusters in the dielectric breakdown model (DBM) by means of iterated conformal mappings. In particular we investigate the fractal dimension and the maximal growth site (measured by the Hoelder exponent alpha_{min} ) as a function of the growth exponent eta of the DBM model. We do not find evidence for a phase transition from fractal to nonfractal growth for a finite eta value. Simultaneously, we observe that the limit of nonfractal growth (D-->1) is consistent with alpha_{min}--… Show more

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Cited by 8 publications
(11 citation statements)
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“…As it tries to maximize the flux into its tip, however, its growth sometimes causes the flux to decline. Indeed, substituting the geodesic growth condition (35) into equations (48), (49) and (50), we find that the variation of the flux reads…”
Section: Maximization Of the Flux Entering The Tipmentioning
confidence: 99%
See 1 more Smart Citation
“…As it tries to maximize the flux into its tip, however, its growth sometimes causes the flux to decline. Indeed, substituting the geodesic growth condition (35) into equations (48), (49) and (50), we find that the variation of the flux reads…”
Section: Maximization Of the Flux Entering The Tipmentioning
confidence: 99%
“…More specifically, at each time step, the slit mapping (25) introduces a new singularity in g, since f ∼ ω − a near the pole a. The probability measure thus becomes non-integrable when η gets larger than 2 (this value actually depends on the infinitesimal map [45,46,48]). The walkers then accumulate on existing tips and the aggregate becomes non-fractal.…”
Section: Random Forcingmentioning
confidence: 99%
“…(The latter contains a figure depicting a simulation of the η = 3 DBM.) However, a later study estimates the dimension of η-DBM in more detail and does not find evidence for a phase transition at η = 4, and concludes that the dimension of η-DBM is about 1.08 when η = 4 [MJB08].…”
Section: Interpretation and Conjecture When η Is Largementioning
confidence: 99%
“…The criticality of the DBM transition is understood in terms of as a non-thermal order parameter. For example, for , it has been suggested that the full collapse to linear clusters occurs at the “critical” value 46,5254 . To address this point, the normalized dimension, , can be used as the non-thermal order parameter of the system, where , when at , and , when as .…”
Section: Discussionmentioning
confidence: 99%
“…As function of the parameter , they go from isotropic and compact structures with , for (Eden clusters); through intricate dendritic-like fractals with , for ; to highly anisotropic linear structures () as . For , the collapse to is expected to occur at 46,47,5254 . Most characterization approaches rely on numerical methods to estimate , with very few theoretical results for 4,5 .…”
Section: Introductionmentioning
confidence: 99%