2006
DOI: 10.1063/1.2390712
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Erratum: “Equation of state of a seven-dimensional hard-sphere fluid. Percus-Yevick theory and molecular-dynamics simulations” [J. Chem. Phys. 120, 9113 (2004)]

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Cited by 16 publications
(32 citation statements)
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“…Interest in studying fluids of hard spheres in d dimensions goes back at least four decades 1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28 and has recently experienced a new boom. 29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,…”
Section: Introductionmentioning
confidence: 99%
“…Interest in studying fluids of hard spheres in d dimensions goes back at least four decades 1,2,3,4,5,6,7,8,9,10,11,12,13,14,15,16,17,18,19,20,21,22,23,24,25,26,27,28 and has recently experienced a new boom. 29,30,31,32,33,34,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51,52,…”
Section: Introductionmentioning
confidence: 99%
“…We have shown that this approach gives the exact solution of the OZ equation with the PY closure. From that perspective, our work extends, on one hand, the Lebowitz solution for 3D-sphere mixtures [80] to higher dimensions and, on the other hand, the PY solution for one-component hyperspheres [3,7,45,62] to the case of mixtures.…”
Section: Discussionmentioning
confidence: 60%
“…Again η f is unknown but we may once more recur to the one-component case. For this system, Colot and Baus [19] have conjectured that (η f /η cp ) 1/d becomes independent of d for high d. Further, from the analysis of the results in d = 3, 4, 5 [16,20], and d = 7 [23] one finds that η f ≈ 1.3. Since at freezing or melting the Helmholtz free energies of the fluid and the solid should be of the same order of magnitude, by considering the former given by the second virial approximation and the latter as obtained from free volume theory with the estimate (η f /η cp ) 1/d ≈ 0.8, we obtain the rough estimate η f ≈ 2.3.…”
mentioning
confidence: 88%
“…Although there had been a few earlier papers [15,16] dealing with hard spheres in dimensions greater than three, it was after the pioneer work of Frisch et al [17] in which they showed that the classical hard-sphere fluid in infinitely many dimensions was amenable to full analytical solution, that studies of high dimensional hard-sphere systems became common over the years [4,18,19,20,21,22,23]. The fact that features such as the freezing transition are present in all dimensionalities (except for d = 1) and the parallel between high spatial dimensions and limiting high density situations that seems to exist in fluids (with the added bonus of greater mathematical simplicity as one increases the number of dimensions) suggest that one can gain insight into the thermodynamic behavior of say three-dimensional systems by looking at a similar problem in higher dimensions.…”
mentioning
confidence: 99%