2015/01/31 by Krzysztof Malarz, K. Malarz
Mathematics · Physics and Astronomy · #Combinatorics #Computer science #Condensed matter physics #Cubic crystal system #Electrical resistivity and conductivity #Lattice (music) #Mathematics #Monte Carlo method #Percolation (cognitive psychology) #Percolation threshold #Physics #Quantum mechanics #Random Matrices and Applications #Simple cubic lattice #Simple random sample #Statistical physics #Statistics #Stochastic processes and statistical mechanics #Theoretical and Computational Physics #cond-mat.stat-mech #k-nearest neighbors algorithm #math-ph #math.MP
paper · pdf · doi:10.1103/physreve.91.043301
published as Phys. Rev. E 91, 043301 (2015) · 5 pages, 3 figures
arxiv created 2015/03/21 · openalex publication_date 2015/04/07 · arxiv updated 2015/04/08 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
In this paper, random-site percolation thresholds for a simple cubic (SC) lattice with site neighborhoods containing next-next-next-nearest neighbors (4NN) are evaluated with Monte Carlo simulations. A recently proposed algorithm with low sampling for percolation thresholds estimation (Bastas et al., arXiv:1411.5834) is implemented for the studies of the top-bottom wrapping probability. The obtained percolation thresholds are pC(4NN)=0.311\phantom\rule0.16em0ex60(12),pC(4NN+NN)=0.150\phantom\rule0.16em0ex40(12),pC(4NN+2NN)=0.159\phantom\rule0.16em0ex50(12),pC(4NN+3NN)=0.204\phantom\rule0.16em0ex90(12),pC(4NN+2NN+NN)=0.114\phantom\rule0.16em0ex40(12),pC(4NN+3NN+NN)=0.119\phantom\rule0.16em0ex20(12),pC(4NN+3NN+2NN)=0.113\phantom\rule0.16em0ex30(12), and pC(4NN+3NN+2NN+NN)=0.100\phantom\rule0.16em0ex00(12), where 3NN, 2NN, and NN stand for next-next-nearest neighbors, next-nearest neighbors, and nearest neighbors, respectively. As an SC lattice with 4NN neighbors may be mapped onto two independent interpenetrated SC lattices but with a lattice constant that is twice as large, the percolation threshold pC(4NN) is exactly equal to pC(NN). The simplified method of Bastas et al. allows for uncertainty of the percolation threshold value pC to be reached, similar to that obtained with the classical method but ten times faster.