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Volumn 56, Issue 1 SUPPL. A, 1997, Pages

Experimental measurement of the persistence exponent of the planar Ising model

Author keywords

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Indexed keywords


EID: 0003033253     PISSN: 1063651X     EISSN: None     Source Type: Journal    
DOI: 10.1103/physreve.56.r40     Document Type: Article
Times cited : (102)

References (38)
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    • to be published
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    • unpublished
    • W. Y. Tam, R. Zeitak, K. Y. Szeto, and J. Stavans (unpublished); B. Levitan and E. Domany (unpublished); for soap bubbles (d > 1), one simply has θ=λ/2=d/2; see C. Sire and S. N. Majumdar, Phys. Rev. E 52, 244 (1995).
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    • unpublished; for soap bubbles (d > 1), one simply has θ=λ/2=d/2;
    • W. Y. Tam, R. Zeitak, K. Y. Szeto, and J. Stavans (unpublished); B. Levitan and E. Domany (unpublished); for soap bubbles (d > 1), one simply has θ=λ/2=d/2; see C. Sire and S. N. Majumdar, Phys. Rev. E 52, 244 (1995).
    • Levitan, B.1    Domany, E.2
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    • note
    • S. J. Cornell (unpublished). Note that the values of θ obtained in the d = 2 Ising simulations are systematically slightly higher than those obtained for the noiseless TDGL. This puzzling fact may be an indication that these two systems are not in the same universality class as far as measuring θ is concerned (see [10] for a discussion in d = 3).
  • 38
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    • Forty points were used in all except one run, where an imperfection in one corner pinned the domain wall. In this case, the 12 points were eliminated that were in the immediate vicinity of the site
    • Forty points were used in all except one run, where an imperfection in one corner pinned the domain wall. In this case, the 12 points were eliminated that were in the immediate vicinity of the site.


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