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Anisotropic diffusion-limited aggregation

M. N. Popescu, H. G. E. Hentschel, and F. Family
Phys. Rev. E 69, 061403 – Published 16 June 2004

Abstract

Using stochastic conformal mappings, we study the effects of anisotropic perturbations on diffusion-limited aggregation (DLA) in two dimensions. The harmonic measure of the growth probability for DLA can be conformally mapped onto a constant measure on a unit circle. Here we map m preferred directions for growth to a distribution on the unit circle, which is a periodic function with m peaks in [π,π) such that the angular width σ of the peak defines the “strength” of anisotropy ϰ=σ1 along any of the m chosen directions. The two parameters (m,ϰ) map out a parameter space of perturbations that allows a continuous transition from DLA (for small enough ϰ) to m needlelike fingers as ϰ. We show that at fixed m the effective fractal dimension of the clusters D(m,ϰ) obtained from mass-radius scaling decreases with increasing ϰ from DDLA1.71 to a value bounded from below by Dmin=32. Scaling arguments suggest a specific form for the dependence of the fractal dimension D(m,ϰ) on ϰ for large ϰ which compares favorably with numerical results.

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  • Received 20 July 2003

DOI:https://doi.org/10.1103/PhysRevE.69.061403

©2004 American Physical Society

Authors & Affiliations

M. N. Popescu1,2,*, H. G. E. Hentschel3,†, and F. Family3,‡

  • 1Max-Planck-Institut für Metallforschung, Heisenbergstrasse 3, D-70569 Stuttgart, Germany
  • 2Institut für Theoretische und Angewandte Physik, Universität Stuttgart, Pfaffenwaldring 57, D-70569 Stuttgart, Germany
  • 3Department of Physics, Emory University, Atlanta, Georgia 30322, USA

  • *Electronic address: popescu@mf.mpg.de
  • Electronic address: phshgeh@physics.emory.edu
  • Electronic address: phyff@emory.edu

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Issue

Vol. 69, Iss. 6 — June 2004

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Images

  • Figure 1
    Figure 1
    (a) Diagrammatic representation of the mappings Φ and ϕ. (b) Change in shape of the probability distribution G(ξ;m,k), Eq. (6), with increasing k for m=3.Reuse & Permissions
  • Figure 2
    Figure 2
    (Color online) Typical clusters (size N=20 000) grown using the modulation G(θ;m,k) with (a) m=3, 4, fixed k=3, and (b) fixed m=6, but different values for k, k=1, and k=10, respectively.Reuse & Permissions
  • Figure 3
    Figure 3
    (a) Average F1(n) as a function of n for clusters grown with k=1, 10, 40, and 80, respectively, and fixed m=6 (log-log plot). Also shown (dashed lines) are both the limit case F1(n)n1DDLA (DLA cluster), where DDLA=1.71, and the proposed lower bound for anisotropic DLA growth, F1(n)n1Dmin, where Dmin=32 [17]. (b) The effective fractal dimension D(m,k), obtained from F1(n)n1D(m,k), as a function of k at fixed m. The points represent the measured values, the lines are just a guide to the eye. The results in both (a) and (b) correspond to the modulation G(θ;m,k).Reuse & Permissions
  • Figure 4
    Figure 4
    (Color online) (a) Superposition of 10 different clusters of size N=105 grown with the modulation G(θ;m,k), the same m=3 and k=1, but different sequences of random numbers. The dotted diamond around the arm centered at ψ=0 shows the approximation for the envelope of one arm of the cluster, and the drawing in the upper right corner shows schematically the geometry of the diamond. (b),(c) Numerical results for (D1)(2D3) as a function of the scaling variable ϰ=mk (for modulation function G) and χ=ε1 (for modulation function G̃), respectively. The dashed lines are just a guide to the eye for the linear behavior in the range of small and large values of ϰ, respectively.Reuse & Permissions
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