Finite-size scaling, dynamic fluctuations, and hyperscaling relation in the Kuramoto model

被引:35
作者
Hong, Hyunsuk [1 ,2 ]
Chate, Hugues [3 ,4 ]
Tang, Lei-Han [4 ,5 ]
Park, Hyunggyu [6 ,7 ]
机构
[1] Chonbuk Natl Univ, Dept Phys, Jeonju 561756, South Korea
[2] Chonbuk Natl Univ, Res Inst Phys & Chem, Jeonju 561756, South Korea
[3] CEA Saclay, CNRS UMR 3680, Serv Phys Etat Condense, F-91191 Gif Sur Yvette, France
[4] Beijing Computat Sci Res Ctr, Beijing 100084, Peoples R China
[5] Hong Kong Baptist Univ, Dept Phys, Kowloon Tong, Hong Kong, Peoples R China
[6] Korea Inst Adv Study, Sch Phys, Seoul 130722, South Korea
[7] Korea Inst Adv Study, QUC, Seoul 130722, South Korea
关键词
PHASE-TRANSITION; POPULATIONS; SYNCHRONIZATION; SYSTEMS;
D O I
10.1103/PhysRevE.92.022122
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
We revisit the Kuramoto model to explore the finite-size scaling (FSS) of the order parameter and its dynamic fluctuations near the onset of the synchronization transition, paying particular attention to effects induced by the randomness of the intrinsic frequencies of oscillators. For a population of size N, we study two ways of sampling the intrinsic frequencies according to the same given unimodal distribution g(omega). In the "random" case, frequencies are generated independently in accordance with g(omega), which gives rise to oscillator number fluctuation within any given frequency interval. In the "regular" case, the N frequencies are generated in a deterministic manner that minimizes the oscillator number fluctuations, leading to quasiuniformly spaced frequencies in the population. We find that the two samplings yield substantially different finite-size properties with clearly distinct scaling exponents. Moreover, the hyperscaling relation between the order parameter and its fluctuations is valid in the regular case, but it is violated in the random case. In this last case, a self-consistent mean-field theory that completely ignores dynamic fluctuations correctly predicts the FSS exponent of the order parameter but not its critical amplitude.
引用
收藏
页数:8
相关论文
共 28 条
[1]   The Kuramoto model:: A simple paradigm for synchronization phenomena [J].
Acebrón, JA ;
Bonilla, LL ;
Vicente, CJP ;
Ritort, F ;
Spigler, R .
REVIEWS OF MODERN PHYSICS, 2005, 77 (01) :137-185
[2]  
[Anonymous], 1975, LECT NOTES PHYS, DOI [DOI 10.1007/BFB0013365, 10.1007/BFb0013365]
[3]  
[Anonymous], NUMERICAL ANAL
[4]   FINITE-SIZE TESTS OF HYPERSCALING [J].
BINDER, K ;
NAUENBERG, M ;
PRIVMAN, V ;
YOUNG, AP .
PHYSICAL REVIEW B, 1985, 31 (03) :1498-1502
[5]   AN INVESTIGATION OF FINITE SIZE SCALING [J].
BREZIN, E .
JOURNAL DE PHYSIQUE, 1982, 43 (01) :15-22
[6]   INTRINSIC FLUCTUATIONS AND A PHASE-TRANSITION IN A CLASS OF LARGE POPULATIONS OF INTERACTING OSCILLATORS [J].
DAIDO, H .
JOURNAL OF STATISTICAL PHYSICS, 1990, 60 (5-6) :753-800
[7]   Susceptibility of large populations of coupled oscillators [J].
Daido, Hiroaki .
PHYSICAL REVIEW E, 2015, 91 (01)
[8]  
Ditto W, 2002, NATURE, V415, P736, DOI 10.1038/415736b
[9]   SCALING AND CRITICAL SLOWING DOWN IN RANDOM-FIELD ISING SYSTEMS [J].
FISHER, DS .
PHYSICAL REVIEW LETTERS, 1986, 56 (05) :416-419
[10]   Kinetic theory of coupled oscillators [J].
Hildebrand, Eric J. ;
Buice, Michael A. ;
Chow, Carson C. .
PHYSICAL REVIEW LETTERS, 2007, 98 (05)