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Diffusion-driven self-assembly of rodlike particles: Monte Carlo simulation on a square lattice
Nikolai I Lebovka1, Yuri Yu Tarasevich2, Volodymyr A Gigiberiya3
1Department of Physical Chemistry of Disperse Minerals, F.D. Ovcharenko Institute of Biocolloidal Chemistry, NAS of Ukraine, Kiev, Ukraine, 03142 and Department of Physics, Taras Shevchenko Kiev National University, Kiev, Ukraine, 01033.
Monte Carlo simulations reveal that rodlike particles self-assemble into diagonal stripe domains. This self-organization behavior is an attractor, but relaxation time increases with lattice size.
Area of Science:
- Statistical Mechanics
- Materials Science
- Computational Physics
Background:
- Studying diffusion-driven self-assembly is crucial for understanding material properties.
- Rodlike particles exhibit complex self-organization behaviors.
- Previous studies have explored particle assembly on lattices.
Purpose of the Study:
- To investigate the diffusion-driven self-assembly of rodlike particles (k-mers) on a 2D lattice.
- To identify the stages and final patterns of self-organization.
- To determine if the observed patterns are attractors and how lattice size affects relaxation time.
Main Methods:
- Monte Carlo simulations were employed to model particle behavior.
- Particles were represented as linear k-mers on a 2D square lattice with periodic boundary conditions.
- Parameters varied included lattice size (L=128 to 2048) and k-mer length (k=2 to 12).
Main Results:
- Distinct self-organization behaviors were observed for short and long k-mers.
- For long k-mers (k≥6), three stages were identified: jamming state destruction, cluster coarsening with labyrinth formation, and diagonal stripe domain formation.
- Diagonal stripe domains were confirmed as an attractor state, regardless of initial configuration.
Conclusions:
- The study elucidates the multi-stage self-assembly process of rodlike particles.
- Diagonal stripe patterns represent a stable attractor state in this system.
- Increased lattice size significantly prolongs the time required to reach the steady state.
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