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For a particularly simple derivation, see also T. W. Burkhardt (to be published)
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T. W. Burkhardt, J. Phys. A 26, L1157 (1993); Y. G. Sinai, Theor. Math. Phys. 90, 219 (1992). For a particularly simple derivation, see also T. W. Burkhardt (to be published).
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It should be noted that Eq. (2) omits certain features of real surfaces. See, e.g., J. Krug, Adv. Phys. 46, 139 (1997): D. Moldovan and L. Golubovic, Phys. Rev. E 61, 6190 (2000).
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It should be noted that Eq. (2) omits certain features of real surfaces. See, e.g., J. Krug, Adv. Phys. 46, 139 (1997): D. Moldovan and L. Golubovic, Phys. Rev. E 61, 6190 (2000).
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S. J. Cornell (private communication).
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Cornell, S.J.1
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0343695539
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private communication
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x = 1 - H has recently been verified by G. Manoj (private communication).
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Manoj, G.1
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