Finite-size scaling analysis and dynamic study of the critical behavior of a model for the collective displacement of self-driven individuals

被引:73
作者
Baglietto, Gabriel [1 ]
Albano, Ezequiel V. [1 ]
机构
[1] Univ Nacl La Plata, Inst Invest Fisicoquim Teor & Aplicadas, CCT La Plata CONICET, Fac Ciencias Exactas, La Plata, Argentina
来源
PHYSICAL REVIEW E | 2008年 / 78卷 / 02期
关键词
D O I
10.1103/PhysRevE.78.021125
中图分类号
O35 [流体力学]; O53 [等离子体物理学];
学科分类号
070204 ; 080103 ; 080704 ;
摘要
The Vicsek model (VM) [T. Vicsek et al., Phys. Rev. Lett. 75, 1226 (1995)], for the description of the collective behavior of self-driven individuals, assumes that each of them adopts the average direction of movement of its neighbors, perturbed by an external noise. A second-order transition between a state of ordered collective displacement (low-noise limit) and a disordered regime (high-noise limit) was found early on. However, this scenario has recently been challenged by Gregory and Chate [G. Gregory and H. Chate, Phys. Rev. Lett. 92, 025702 (2004)] who claim that the transition of the VM may be of first order. By performing extensive simulations of the VM, which are analyzed by means of both finite-size scaling methods and a dynamic scaling approach, we unambiguously demonstrate the critical nature of the transition. Furthermore, the complete set of critical exponents of the VM, in d=2 dimensions, is determined. By means of independent methods - i.e., stationary and dynamic measurements - we provide two tests showing that the standard hyper-scaling relationship dv-2 beta = gamma holds, where beta, nu, and gamma are the order parameter, correlation length, and "susceptibility" critical exponents, respectively. Furthermore, we established that at criticality, the correlation length grows according to xi similar to t(1/z), with z similar or equal to 1.27(3), independently of the degree of order of the initial configuration, in marked contrast with the behavior of the XY model.
引用
收藏
页数:9
相关论文
共 67 条
[1]   Comment on "Dynamic behavior of anisotropic nonequilibrium driving lattice gases" - Reply [J].
Albano, EV ;
Saracco, G .
PHYSICAL REVIEW LETTERS, 2004, 92 (02)
[2]   Dynamic Behavior of anisotropic nonequilibrium driving lattice gases [J].
Albano, EV ;
Saracco, G .
PHYSICAL REVIEW LETTERS, 2002, 88 (14) :4
[3]   Self-organized collective displacements of self-driven individuals [J].
Albano, EV .
PHYSICAL REVIEW LETTERS, 1996, 77 (10) :2129-2132
[4]  
Barber M.N., 1983, PHASE TRANSITIONS CR, V8, P146
[5]   Experimental evidences of a structural and dynamical transition in fish school [J].
Becco, C ;
Vandewalle, N ;
Delcourt, J ;
Poncin, P .
PHYSICA A-STATISTICAL MECHANICS AND ITS APPLICATIONS, 2006, 367 (487-493) :487-493
[6]   Chemomodulation of cellular movement, collective formation of vortices by swarming bacteria, and colonial development [J].
BenJacob, E ;
Cohen, I ;
Czirok, A ;
Vicsek, T ;
Gutnick, DL .
PHYSICA A-STATISTICAL MECHANICS AND ITS APPLICATIONS, 1997, 238 (1-4) :181-197
[7]   Boltzmann and hydrodynamic description for self-propelled particles [J].
Bertin, Eric ;
Droz, Michel ;
Gregoire, Guillaume .
PHYSICAL REVIEW E, 2006, 74 (02)
[8]  
Binder K., 2002, GUIDE MONTE CARLO SI
[9]  
Binner JJ., 1992, The theory of critical phenomena, an introduction to the Renormalization Group
[10]   Space dimension and scaling in fish school-size distributions [J].
Bonabeau, E ;
Dagorn, L ;
Freon, P .
JOURNAL OF PHYSICS A-MATHEMATICAL AND GENERAL, 1998, 31 (44) :L731-L736