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Volumn 67, Issue 3, 2003, Pages 4-

Dynamic critical behavior of the [Formula presented] model in small-world networks

Author keywords

[No Author keywords available]

Indexed keywords


EID: 85037232477     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevE.67.036118     Document Type: Article
Times cited : (6)

References (36)
  • 12
  • 15
    • 85037187171 scopus 로고    scopus 로고
    • P. Holme, e-print cond-mat/030113.
    • Holme, P.1
  • 27
    • 85037218211 scopus 로고    scopus 로고
    • d dimensional regular lattices, we have (Formula presented) and (Formula presented) with the linear size of the system L, the correlation length (Formula presented) and the correlation volume (Formula presented) Accordingly, at (Formula presented) we have (Formula presented) Since (Formula presented) diverges as (Formula presented) we also have (Formula presented) For systems where the correlation length is not well defined, but the correlation volume is well defined (as in the present work), (Formula presented) and (Formula presented) need to be measured to detect the dynamic and static universality class of the system. In the mean-field systems corresponding to (Formula presented) (Formula presented) and (Formula presented) are expected
    • In d dimensional regular lattices, we have (Formula presented) and (Formula presented) with the linear size of the system L, the correlation length (Formula presented) and the correlation volume (Formula presented) Accordingly, at (Formula presented) we have (Formula presented) Since (Formula presented) diverges as (Formula presented) we also have (Formula presented) For systems where the correlation length is not well defined, but the correlation volume is well defined (as in the present work), (Formula presented) and (Formula presented) need to be measured to detect the dynamic and static universality class of the system. In the mean-field systems corresponding to (Formula presented) (Formula presented) and (Formula presented) are expected.
  • 32
    • 0000365878 scopus 로고    scopus 로고
    • we obtain a value (Formula presented) closer to 0.5
    • If we assume a logarithmic correction to the characteristic length scale (Formula presented) as it was suggested by A.J. Bray, A.J. Briant, and D.K. Jervis, Phys. Rev. Lett. 84, 1503 (2000), we obtain a value (Formula presented) closer to 0.5.
    • (2000) Phys. Rev. Lett. , vol.84 , pp. 1503
    • Bray, A.J.1    Briant, A.J.2    Jervis, D.K.3
  • 33
    • 85037196302 scopus 로고    scopus 로고
    • To arrive at the result (Formula presented) we set the threshold for breakdown of scaling (i.e., where we would have needed yet larger system sizes) to (Formula presented) and average all points for larger P values
    • To arrive at the result (Formula presented) we set the threshold for breakdown of scaling (i.e., where we would have needed yet larger system sizes) to (Formula presented) and average all points for larger P values.
  • 35
    • 85037190682 scopus 로고    scopus 로고
    • W.H. Press, S.A. Teukolsky, W.T. Vetterling, and B.P. Flannery, Numerical Recipes in C: The Art of Scientific Computing, 2nd ed. (Cambridge University Press, Cambridge, 1992)
    • W.H. Press, S.A. Teukolsky, W.T. Vetterling, and B.P. Flannery, Numerical Recipes in C: The Art of Scientific Computing, 2nd ed. (Cambridge University Press, Cambridge, 1992).
  • 36
    • 85037204072 scopus 로고    scopus 로고
    • B. Efron, The Jackknife, the Bootstrap, and Other Resampling Plans (SIAM, Philadelphia, 1982)
    • B. Efron, The Jackknife, the Bootstrap, and Other Resampling Plans (SIAM, Philadelphia, 1982).


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.