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85034554093
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note
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In [9], the behavior described by equation (2) has been related to the non-extensivity of the entropy proposed in [11]. Indeed, the exponent a can be shown to be α = 1/(1 - q) where q is the extensivity parameter (q = 1 corresponding to the extensive case). We will not discuss this point further in this paper.
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85034557084
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note
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A new set of measurements, to be presented elsewhere [14], furnishes an extrapolation for big N of the exponent Q to be close to 0.4.
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21
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85034546185
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note
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In [1], the authors introduced also a "tunable" version of the parallel BS model. In this paper we concentrate only on the non-tunable version.
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25
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0031206179
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H. Hinrichsen, J.S. Weitz, E. Domany, J. Stat. Phys. 88, 617 (1997); P. Grassberger, J. Stat. Phys. 79, 13 (1995).
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Hinrichsen, H.1
Weitz, J.S.2
Domany, E.3
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26
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21844506820
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H. Hinrichsen, J.S. Weitz, E. Domany, J. Stat. Phys. 88, 617 (1997); P. Grassberger, J. Stat. Phys. 79, 13 (1995).
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Grassberger, P.1
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note
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In the evolution of both system and copy the same random numbers are used.
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29
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85034555434
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note
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It is interesting to note that in the PBS the effect of the map is much smoother than in the case of the extremal BS [18]. This difference is certainly due to the fact that the effect of time correlation is "washed" out easier if the number of updated sites is big.
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