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A. Vespignani, R. Dickman, M.A. Muñoz, S. Zapperi, Phys. Rev. E 62, 4564 (2000).
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Phys. Rev. E
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Vespignani, A.1
Dickman, R.2
Muñoz, M.A.3
Zapperi, S.4
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14
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0000563105
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L.P. Kadanoff, S.R. Nagel, L. Wu, S. Zhou, Phys. Rev. A 39, 6524 (1989).
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Phys. Rev. A
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Kadanoff, L.P.1
Nagel, S.R.2
Wu, L.3
Zhou, S.4
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15
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85037510499
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In the original Zhang model [9] the energy increment δ in constant; the random increment used in this work leads to the same critical behavior, but renders the algorithm faster [11]
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In the original Zhang model [9] the energy increment δ in constant; the random increment used in this work leads to the same critical behavior, but renders the algorithm faster [11].
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16
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0003672584
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edited by A. McKane et al. Plenum, New York
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G. Grinstein, in Scale Invariance, Interfaces and Nonequilibrium Dynamics, NATO Advanced Study Institute, Series B: Physics, Vol. 344, edited by A. McKane et al. (Plenum, New York, 1995); A. Vespignani, S. Zapperi, Phys. Rev. E 57, 6345 (1998).
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(1995)
Scale Invariance, Interfaces and Nonequilibrium Dynamics, NATO Advanced Study Institute, Series B: Physics
, vol.344
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Grinstein, G.1
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17
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4243736448
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G. Grinstein, in Scale Invariance, Interfaces and Nonequilibrium Dynamics, NATO Advanced Study Institute, Series B: Physics, Vol. 344, edited by A. McKane et al. (Plenum, New York, 1995); A. Vespignani, S. Zapperi, Phys. Rev. E 57, 6345 (1998).
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(1998)
Phys. Rev. E
, vol.57
, pp. 6345
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Vespignani, A.1
Zapperi, S.2
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19
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85037516073
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t represents the dynamic critical exponent z
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t represents the dynamic critical exponent z.
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20
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85037495465
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When computing the moments, one has to be aware of the limitations of the validity of equation (2) for large q. At large q, the maximum contribution in the average (2) corresponds to the largest avalanches, of which one has the poorest statistics. Therefore, the moment's estimation for large q is affected by large statistical errors
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When computing the moments, one has to be aware of the limitations of the validity of equation (2) for large q. At large q, the maximum contribution in the average (2) corresponds to the largest avalanches, of which one has the poorest statistics. Therefore, the moment's estimation for large q is affected by large statistical errors.
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21
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85037493660
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cond-mat/0003420
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A. Vázquez, cond-mat/0003420.
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Vázquez, A.1
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22
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85037497906
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Note the essential difference between this model and the Manna model in the limit of infinite threshold recently introduce by Lübeck [S. Lübeck, cond-mat/0008304]
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Note the essential difference between this model and the Manna model in the limit of infinite threshold recently introduce by Lübeck [S. Lübeck, cond-mat/0008304].
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