Book contents
- Frontmatter
- Contents
- Preface
- Notation guide
- PART 1 Introduction
- PART 2 Nonequilibrium roughening
- PART 3 Interfaces in random media
- PART 4 Molecular beam epitaxy
- 12 Basic phenomena of MBE
- 13 Linear theory of MBE
- 14 Nonlinear theory for MBE
- 15 Discrete models for MBE
- 16 MBE experiments
- 17 Submonolayer deposition
- 18 The roughening transition
- 19 Nonlocal growth models
- 20 Diffusion bias
- PART 5 Noise
- PART 6 Advanced topics
- PART 7 Finale
- APPENDIX A Numerical recipes
- APPENDIX B Dynamic renormalization group
- APPENDIX C Hamiltonian description
- Bibliography
- Index
19 - Nonlocal growth models
Published online by Cambridge University Press: 23 December 2009
- Frontmatter
- Contents
- Preface
- Notation guide
- PART 1 Introduction
- PART 2 Nonequilibrium roughening
- PART 3 Interfaces in random media
- PART 4 Molecular beam epitaxy
- 12 Basic phenomena of MBE
- 13 Linear theory of MBE
- 14 Nonlinear theory for MBE
- 15 Discrete models for MBE
- 16 MBE experiments
- 17 Submonolayer deposition
- 18 The roughening transition
- 19 Nonlocal growth models
- 20 Diffusion bias
- PART 5 Noise
- PART 6 Advanced topics
- PART 7 Finale
- APPENDIX A Numerical recipes
- APPENDIX B Dynamic renormalization group
- APPENDIX C Hamiltonian description
- Bibliography
- Index
Summary
Most of this book deals with local growth processes, for which the growth rate depends on the local properties of the interface. For example, the interface velocity in the BD model depends only on the height of the interface and its nearest neighbors. However, there are a number of systems for which nonlocal effects contribute to the interface morphology and growth velocity. Such growth processes cannot be described using local growth equations, such as the KPZ equation; if we attempt to do so, we must include nonlocal effects. In this chapter we discuss phenomena that lead to nonlocal effects, and we also discuss models describing nonlocal growth processes.
Diffusion-limited aggregation
Probably the most famous cluster growth model is diffusion-limited aggregation (DLA). The model is illustrated in Fig. 19.1. We fix a seed particle on a central lattice site and release another particle from a random position far from the seed. The released particle moves following a Brownian trajectory, until it reaches one of the four nearest neighbors of the seed, whereupon it sticks, forming a two-particle cluster. Next we release a new particle which can stick to any of the six perimeter sites of this two-particle cluster. This process is then iterated repeatedly. In Fig. 19.2, we show clusters resulting from the deposition of 5 × 105, 5 × 106, and 5 × 107 particles.
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- Fractal Concepts in Surface Growth , pp. 209 - 230Publisher: Cambridge University PressPrint publication year: 1995