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3
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4243056062
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B. Nienhuis, A. N. Berker, E. K. Riedel, and M. Schick, Phys. Rev. Lett. 43, 737 (1979).
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Nienhuis, B.1
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Schick, M.4
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6
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0001786512
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See, edited by C. Domb and J. L. Lebowitz, Academic, New York
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See S. Dietrich, in Phase Transitions and Critical Phenomena, edited by C. Domb and J. L. Lebowitz (Academic, New York, 1988), Vol. 12, p. 1.
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Phase Transitions and Critical Phenomena
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Dietrich, S.1
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0001312603
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F. Iglói, L. Turban, D. Karevski, and F. Szalma, Phys. Rev. B 56, 11 031 (1997).
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Phys. Rev. B
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Iglói, F.1
Turban, L.2
Karevski, D.3
Szalma, F.4
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22
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0042492825
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For a review on the Potts model, see
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For a review on the Potts model, seeF. Y. Wu, Rev. Mod. Phys. 54, 235 (1982).
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Rev. Mod. Phys.
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Wu, F.Y.1
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28
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85038306548
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Actually, in the large-(formula presented) limit, (formula presented) is to be understood as the singular part of (formula presented) according to Eq. (3.16)
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Actually, in the large-(formula presented) limit, (formula presented) is to be understood as the singular part of (formula presented) according to Eq. (3.16).
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31
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85038337672
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Since the sequence is not symmetric, the Fibonacci Hamiltonian is only approximately self-dual. Nevertheless, the critical point remains located at (formula presented)
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Since the sequence is not symmetric, the Fibonacci Hamiltonian is only approximately self-dual. Nevertheless, the critical point remains located at (formula presented)
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33
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0000510446
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S. Ostlund, R. Pandit, D. Rand, H. J. Schellnhuber, and E. D. Siggia, Phys. Rev. Lett. 50, 1873 (1983).
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Phys. Rev. Lett.
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Ostlund, S.1
Pandit, R.2
Rand, D.3
Schellnhuber, H.J.4
Siggia, E.D.5
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37
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0003582444
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edited by A. Dold and B. Eckmann, Lecture Notes in Mathematics, Springer, Berlin
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M. Queffélec, in Substitutional Dynamical Systems-Spectral Analyses, edited by A. Dold and B. Eckmann, Lecture Notes in Mathematics, Vol. 1294 (Springer, Berlin, 1987).
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Substitutional Dynamical Systems-Spectral Analyses
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Queffélec, M.1
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41
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85038269917
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Actually, the exact calculation of the exponent (formula presented) was done in Ref. 16 for a directed walk problem. The aperiodic modulation of the weights corresponds in the present problem to the two-letter substitutions obtained by replacing A by (formula presented) and B by (formula presented) in the period-doubling sequence. One expects the same critical behavior since the wandering exponent is not modified by this decoration of the sequence. This is supported by numerical data
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Actually, the exact calculation of the exponent (formula presented) was done in Ref. 16 for a directed walk problem. The aperiodic modulation of the weights corresponds in the present problem to the two-letter substitutions obtained by replacing A by (formula presented) and B by (formula presented) in the period-doubling sequence. One expects the same critical behavior since the wandering exponent is not modified by this decoration of the sequence. This is supported by numerical data.
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