Bond percolation in distorted square and triangular lattices

This article presents a Monte Carlo study on bond percolation in distorted square and triangular lattices. The distorted lattices are generated by dislocating the sites from their regular positions. The amount and direction of the dislocations are random, but can be tuned by the distortion parameter α. Once the sites are dislocated, the bond lengths δ between the nearest neighbors change. A bond can only be occupied if its bond length is less than a threshold value called the connection threshold d. It is observed that when the connection threshold is greater than the lattice constant (assumed to be 1), the bond percolation threshold p_{b} always increases with distortion. For d≤1, no spanning configuration is found for the square lattice when the lattice is distorted, even very slightly. On the other hand, the triangular lattice not only spans for d≤1, it also shows a decreasing trend for p_{b} in the low-α range. These variation patterns have been linked with the average coordination numbers of the distorted lattices. A critical value d_{c} for the connection threshold has been defined as the value of d below which no spanning configuration can be found, even after occupying all the bonds satisfying the connection criterion δ≤d. The behavior of d_{c}(α) is markedly different for the two lattices.

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Publication Details

Journal
Physical review. E
Published
2025-10-09
DOI
https://doi.org/10.1103/8s5c-nw9z
Primary Topic
Theoretical and Computational Physics
Type
article
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article

Bond percolation in distorted square and triangular lattices

Ankur Sensharma, Sayantan Mitra, Robert M. Ziff, Bishnu Bhowmik
Physical review. E
Theoretical and Computational Physics
article

Bond percolation in distorted square and triangular lattices

Ankur Sensharma, Sayantan Mitra, Robert M. Ziff, Bishnu Bhowmik
article en

Abstract

This article presents a Monte Carlo study on bond percolation in distorted square and triangular lattices. The distorted lattices are generated by dislocating the sites from their regular positions. The amount and direction of the dislocations are random, but can be tuned by the distortion parameter α. Once the sites are dislocated, the bond lengths δ between the nearest neighbors change. A bond can only be occupied if its bond length is less than a threshold value called the connection threshold d. It is observed that when the connection threshold is greater than the lattice constant (assumed to be 1), the bond percolation threshold p_{b} always increases with distortion. For d≤1, no spanning configuration is found for the square lattice when the lattice is distorted, even very slightly. On the other hand, the triangular lattice not only spans for d≤1, it also shows a decreasing trend for p_{b} in the low-α range. These variation patterns have been linked with the average coordination numbers of the distorted lattices. A critical value d_{c} for the connection threshold has been defined as the value of d below which no spanning configuration can be found, even after occupying all the bonds satisfying the connection criterion δ≤d. The behavior of d_{c}(α) is markedly different for the two lattices.

Physical review. EVol. 112(4)
Indian Institute of Science Education and Research Kolkata (IN), University of Michigan (US), University of Gour Banga (IN)
Openalex Percentile: Top 84%
Theoretical and Computational Physics
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