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A general review of such methods will appear in Advances in Chemical Physics: Monte Carlo Methods in Chemical Physics, edited by D. Ferguson, J. I. Siepmann, and D. Truhlar, presumably later this year. See also: J. P. Valleau, J. Comput. Phys. 96, 193 (1991); N. V. Brilliantov and J. P. Valleau, J. Chem. Phys. (in press).
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A general review of such methods will appear in Advances in Chemical Physics: Monte Carlo Methods in Chemical Physics, edited by D. Ferguson, J. I. Siepmann, and D. Truhlar, presumably later this year. See also: J. P. Valleau, J. Comput. Phys. 96, 193 (1991); N. V. Brilliantov and J. P. Valleau, J. Chem. Phys. (in press).
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A general review of such methods will appear in Advances in Chemical Physics: Monte Carlo Methods in Chemical Physics, edited by D. Ferguson, J. I. Siepmann, and D. Truhlar, presumably later this year. See also: J. P. Valleau, J. Comput. Phys. 96, 193 (1991); N. V. Brilliantov and J. P. Valleau, J. Chem. Phys. (in press).
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J. Chem. Phys. (in Press)
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Brilliantov, N.V.1
Valleau, J.P.2
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note
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The fitting function had a "double-Padé form. That is, it was the ratio of double polynomials in √T* and √p*. Each polynomial ranged up to fifth order in the former and sixth order in the latter (up to 60 adjustable parameters); over a decent range of these orders the fits are excellent, and are insensitive to the order. Data for free energy at several hundred states was fitted. [While this funcitonal form could not actually give a true Ising divergence for an infinite system, it is expected to be sufficiently flexible to reproduce well the behavior of a finite system, and does so for other small systems we have studied (Ref. 9).]
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note
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c quite close to that estimated by Caillol et al., but that may be accidental.)
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