摘要The percolation-like phase transition of mobile individuals is studied on weighted scale-free (WSF) networks, in which the maximum occupancy at each node is one individual (i.e. hard core interaction) and individuals can move to neighbor void node. Especially, the condition for the existence of a spanning cluster of individuals (a connected cluster of neighbor nodes occupied by individuals that span the entire systems) is investigated and it is found that there exists a critical value of weight coupling parameter βc, above which the density threshold of individuals is zero and below which the density threshold is larger than zero for WSF networks in the thermodynamic limit N→∞. Furthermore, the finite size scaling analysis show that for certain value β, the percolation transition of mobile individuals on a WSF network belongs to the same universality class of regular random graph percolation.
Abstract:The percolation-like phase transition of mobile individuals is studied on weighted scale-free (WSF) networks, in which the maximum occupancy at each node is one individual (i.e. hard core interaction) and individuals can move to neighbor void node. Especially, the condition for the existence of a spanning cluster of individuals (a connected cluster of neighbor nodes occupied by individuals that span the entire systems) is investigated and it is found that there exists a critical value of weight coupling parameter βc, above which the density threshold of individuals is zero and below which the density threshold is larger than zero for WSF networks in the thermodynamic limit N→∞. Furthermore, the finite size scaling analysis show that for certain value β, the percolation transition of mobile individuals on a WSF network belongs to the same universality class of regular random graph percolation.
[1] Albert R and Barabási A L 2002 Rev. Mod. Phys. 74 47
[2] Dorogovtsev S N, Goltsev A V and Mendes J F F 2008 Rev. Mod. Phys. 80 1275
[3] Cohen R, Erez K, Ben-Avraham D and Havlin S 2000 Phys. Rev. Lett. 85 4626
[4] Newman M E J 2002 Phys. Rev. Lett. 89 208701
[5] Goltsev A V, Dorogovtsev S N and Mendes J F F 2008 Phys. Rev. E 78 051105
[6] Serrano M Á and Boguñá M 2006 Phys. Rev. Lett. 97 088701
[7] Moreira A A, Andrade J S, Herrmann H J and Indekeu J O 2009 Phys. Rev. Lett. 102 018701
[8] Liu Z 2010 Phys. Rev. E 81 016110
[9] Yang H X, Wang W X and Wang B H 2010 arXiv:1005.5453
[10] Barrat A, Barthélemy M, Pastor-Satorras R and Vespignani A 2004 Proc. Natl. Acad. Sci. USA 101 3747
[11] Wu A C, Xu X J, Wu Z X, and Wang Y H 2007 Chin. Phys. Lett. 24 577
[12] Colizza V and Vespignani A 2008 J. Theor. Biol. 251 450
[13] Catanzaro M, Boguñ á M and Pastor-Satorras R 2005 Phys. Rev. E 71 027103
[14] Catanzaro M, Boguñ á M and Pastor-Satorras R 2005 Phys. Rev. E 71 056104
[15] Weber S and Porto M 2006 Phys. Rev. E 74 046108
[16] Wu A C, Xu X J, Mendes J F F and Wang Y H 2008 Phys. Rev. E 78 047101
[17] Stauffer D and Aharony A 1994 Introduction to Percolation Theory (New York: Taylor & Frrancis)