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Random Laplacian Growth and Laplacian Erosion

Random Laplacian Growth and Laplacian Erosion. Yup Kim With S. Y. Yoon and S. H. Choi KyungHee University. 1. Why Laplacian? a) Normal Random Walk b) Ballistic Motion c) Biased Random Walk. ( Diffusion Equation ). (Completely Drifted). (Drifted-Diffusion Equation). Click.

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Random Laplacian Growth and Laplacian Erosion

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  1. Random Laplacian Growth and Laplacian Erosion Yup Kim With S. Y. Yoon and S. H. Choi KyungHee University

  2. 1. Why Laplacian? • a) Normal Random Walk • b) Ballistic Motion • c) Biased Random Walk ( Diffusion Equation ) (Completely Drifted) (Drifted-Diffusion Equation) Click

  3. 2. Three Paradigms for Random, • Irreversible and Nonequilibrium Growth • a) Ballistic Deposition • 1) No Anomalous Internal Struture • 2) Nontrivial Surface Structure • (Dynamical Scaling Law : =1/2, =1/3, z=3/2 (1d)) • KPZ equation Click

  4. b) Diffusion-Limited Deposition 1) finitely-ramified fractal structure 2) Click

  5. c) Eden Growth (Dynamical Scaling Law : =1/2, =1/3, z=3/2 (1d)) KPZ equation Click

  6. Family model Ballistic Erosion • 3. Corresponding Erosion Models • to the Three Paradigms • a) Ballistic Erosion • (Dynamical Scaling Law : =1/2, =1/4, z=2 (1d)) • EW Equation : Linear Equation Click

  7. b) Diffusion-Limited Erosion Model • (Dynamical Scaling Law : z=1) • c) Anti-Eden Model •  Critically the same as original Eden Model Click Eden Model Anti-Eden Model

  8. Abandoned particle Killing line yk Starting line (1-Pb)/3 (1-Pb)/3 (1-Pb)/3 ys Pb Hopping Probability ymax 4. Biased Diffusion Limited Erosion a) Model L

  9. b) Corresponding Continuum Equation and Scaling Property <(x, t)>=0 (Dynamical Scaling Law : z=1)

  10. c) Simulation Results Pb = 0.25 (DLD) Dynamic Scaling Law : z = 1

  11. Pb = 0.26  = 0.11 Dynamic Scaling Law : z = 1.6

  12. Pb = 0.73  = 0.51 Dynamic Scaling Law :  = 0.51 (1/2),  = 0.24 (1/4), z = 2.1 (2)

  13.  Scaling Property Summary Growth exponent  Rougheness exponent  Dynamic exponent z

  14. Pb = 0.2 Dynamic Scaling Law : z = 1

  15. d) Summary Biased diffusion Limited Erosions have three regimes.  Regime I : Pb 0.16 : smooth phase (no roughening)  Regime II : 0.17  Pb  0.25 : z=1  Regime III : Pb  0.25 : z2 (EW universality class) The crossover from regime II to regime III is very sudden.

  16. DF 0 2 0.5 1.89 ± 0.01 1 1.75 ±0.02 2 ~1.6a 5. Dielectric Breakdown Model and Anti-dielectric Breakdown Model a) Dielectric Breakdown Model Laplacian Equation (Slow process) Boundary Condition :  (x, y, t) = 0and  (x, yb, t) = 1  Relaxation Method Growth Probability

  17.  (x, yb, t) = 1 yb (x,h)  (x, y, t) = 0 b) Anti-dielectric Breakdown Model Erosion Probability

  18. c) Simulation Results = 1  비교 Diffusion Limited Annihilation (Pb= 0.25)

  19. < 1   = 0 (Anti-Eden Model)  = 0.33  = 0.49 Dynamic Scaling Law :  = 1/2,  = 1/3, z = 3/2(1.49)

  20.   = 0.01  = 0.48  = 0.33 Dynamic Scaling Law :  = 0.48 (1/2),  = 0.33 (1/3), z = 1.45 (3/2)

  21.   = 0.1  = 0.30  = 0.18 Crossover Regime : z = 1.67

  22.  >1 ( = 2)   = 0.5 Dynamic Scaling Law : z = 1

  23. d) Summary   0 anti-Eden model (KPZ equation) 0.1<  < 0.5(?) Crossover Regime(?) EW or KPZ universality class(?) 0.5   2 Linear growth equation(Diffusion Limited Erosion) Dynamic exponent, z=1  >2(?)   : smooth phase (No roughening)

  24. Erosion Model with Drifted-Laplacian Equation * ? + Boundary Condition D=0, Ballistic Motion ? Poisson Equation ? Source term ? 6. Final Discussion

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