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Asymmetric Walkway: A Novel Behavioral Assay for Studying Asymmetric Locomotion
Published on: January 15, 2016
Nature of the collapse transition in interacting self-avoiding trails
Tiago J Oliveira1, Jürgen F Stilck2
1Departamento de Física, Universidade Federal de Viçosa, 36570-900 Viçosa, Minas Gerais, Brazil.
The interacting self-avoiding trail (ISAT) model reveals complex phase diagrams on lattices. This study identifies distinct phases and transitions, offering insights into polymer collapse phenomena.
Area of Science:
- Statistical Mechanics
- Polymer Physics
- Phase Transitions
Background:
- The interacting self-avoiding trail (ISAT) model is crucial for understanding polymer behavior.
- Previous studies on lattices have shown varied phase diagrams and transition behaviors.
Purpose of the Study:
- To investigate the phase diagrams of the ISAT model on Bethe and Husimi lattices.
- To analyze the effects of monomer capacity (K) and site-visit weights (ωᵢ) on phase transitions.
- To compare ISAT behavior with interacting self-avoiding walks and explain observed differences in collapse transitions.
Main Methods:
- Exact grand-canonical solutions were derived for the ISAT model.
- The study considered lattices with general coordination (q) and specific square lattices (q=4).
- Monomer capacity (K) and site-visit weights (ωᵢ) were incorporated into the model.
Main Results:
- Rich phase diagrams were found, featuring nonpolymerized, regular polymerized, and dense polymerized phases.
- Transitions were characterized as continuous and discontinuous, with complex structures for higher q and K values.
- For q=4, K=2, the collapse transition was identified as a bicritical point, with the collapsed phase being solidlike.
Conclusions:
- The ISAT model exhibits complex phase behavior on Bethe and Husimi lattices, influenced by lattice coordination and monomer capacity.
- The findings provide a potential explanation for differences in collapse transitions between ISATs and self-avoiding walks.
- The study maps phase diagrams to the canonical ensemble, facilitating comparison with simulation results on regular lattices.
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