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note
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The present spherical model defined by Eq. (26) is different from the O(n) spherical model discussed in previous papers [11]. In that case both the order parameter and the U field were vector fields coupled bilinearly. However, the two models in the infinite-volume limit and in the limit of infinite components generate identical equations for the average fields and their correlations, although the physical interpretation remains different for the two models.
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25
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36049054483
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Stanley has shown the equivalence of the spherical model and an n-component spin model in the limit of n → ∞ in the case of translationally invariant systems. H.E. Stanley, Phys. Rev. 76, 718 (1968).
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The equilibrium properties of interfaces have been studied in the mode-coupling approximation by U. Marini Bettolo Marconi and B.L. Gyorffy, Physica A 159, 221 (1989); Phys. Rev. A 41, 6732 (1990).
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5244330541
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The equilibrium properties of interfaces have been studied in the mode-coupling approximation by U. Marini Bettolo Marconi and B.L. Gyorffy, Physica A 159, 221 (1989); Phys. Rev. A 41, 6732 (1990).
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30
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note
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2 term and U ø in Eq. (26) have not been chosen independently, as assumed in Ref. [11], but their ratio was fixed to guarantee the correct energy balance as explained in Sees. II and I.
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Although the notion of a spinodal line signaling a sharp transition from a nucleation mechanism to a spinodal decomposition mechanism is not exact in systems with finite-range interactions and the transition is gradual, still the concept of spinodal has a heuristic value [see, for example, the article by Binder about spinodal decomposition: K. Binder, in Materials Science and Technology, edited by R.W. Cahn, P. Haasen, and E.J. Kramer (VCH, Weinheim, 1991)].
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