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Density functional theory of nonuniform polyatomic systems. II. Rational closures for integral equations
1.D. Chandler, J. D. McCoy, and S. J. Singer, J. Chem. Phys. 85, 5971 (1986), referred to as paper I.
2.J. K. Percus, in Studies in Statistical Mechanics VIII, edited by E. W. Montroll and J. L. Lebowitz (North‐Holland, Amsterdam, 1982). See also additional references cited in paper I.
3.L. J. Bartolotti and P. K. Achary, J. Chem. Phys. 77, 4576 (1982).
4.T. V. Ramakrishnan and M. Yussouff, Phys. Rev. B 19, 2775 (1979);
4.A. D. J. Haymet and D. Oxtoby, J. Chem. Phys. 74, 2559 (1981).
5.F. Hirata and P. J. Rossky, Chem. Phys. Lett. 83, 329 (1981);
5.F. Hirata, B. M. Pettitt, and P. J. Rossky, J. Chem. Phys. 77, 509 (1982).
6.J. K. Percus, in The Equilibrium Theory of Classical Fluids, edited by H. L. Frisch and J. L. Lebowitz (Benjamin, New York, 1964).
7.The original RISM equation [D. Chandler and H. C. Andersen, J. Chem. Phys. 57, 1930 (1972)]
7.applicable only to hard core molecules, does successfully interpolate, but with the end points described by the Percus‐Yevick closure for hard spheres
7.[J. K. Percus and G. Yevick, Phys. Rev. A 110, 1 (1958)].
7.See B. M. Ladanyi and D. Chandler, J. Chem. Phys. 62, 4308 (1975). But extensions to systems with continuous potentials (e.g., the closures suggested in Ref. 5) do not sensibly interpolate.
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