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5
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B.J. Kim, H. Hong, P. Holme, G.S. Jeon, P. Minnhagen, and M.Y. Choi, Phys. Rev. E 64, 056135 (2001).
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P. Holme, e-print cond-mat/030113.
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Holme, P.1
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4244146692
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B.J. Kim, P. Minnhagen, S.K. Oh, and J.S. Chung, Phys. Rev. B 64, 024406 (2001).
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5744249209
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N. Metropolis, A.W. Rosenbluth, M.N. Rosenbluth, A.H. Teller, and E. Teller, J. Chem. Phys. 21, 1087 (1953).
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Metropolis, N.1
Rosenbluth, A.W.2
Rosenbluth, M.N.3
Teller, A.H.4
Teller, E.5
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27
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85037218211
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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
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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.
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32
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0000365878
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we obtain a value (Formula presented) closer to 0.5
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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.
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Phys. Rev. Lett.
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Bray, A.J.1
Briant, A.J.2
Jervis, D.K.3
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33
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85037196302
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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
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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.
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34
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43949163997
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H.E. Stanley, S.V. Buldyrev, A.L. Goldberger, S. Havlin, C.-K. Peng, and M. Simons, Physica A 200, 4 (1993).
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Stanley, H.E.1
Buldyrev, S.V.2
Goldberger, A.L.3
Havlin, S.4
Peng, C.-K.5
Simons, M.6
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35
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85037190682
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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)
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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).
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36
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85037204072
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B. Efron, The Jackknife, the Bootstrap, and Other Resampling Plans (SIAM, Philadelphia, 1982)
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B. Efron, The Jackknife, the Bootstrap, and Other Resampling Plans (SIAM, Philadelphia, 1982).
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