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48
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85033069783
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note
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0 is too small to distinguish between large clusters and the small clusters of 2-3 atoms which occur in the cavity regions.
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49
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85033072546
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note
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c, consistent with the conclusion that the majority of cluster rearrangements occur by slow collective motions.
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51
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85033054438
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av(t), and we have included the average atoms in the high density count for simplicity
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av(t), and we have included the average atoms in the high density count for simplicity.
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54
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36749110571
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W. C. Swope, H. C. Andersen, P. H. Berens, and K. R. Wilson, J. Chem. Phys. 76, 637 (1982).
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Berens, P.H.3
Wilson, K.R.4
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56
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36749107989
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M. R. Mruzik, F. F. Abraham, D. E. Schreiber, and G. M. Pound, J. Chem. Phys. 64, 481 (1976).
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Mruzik, M.R.1
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Pound, G.M.4
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57
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85033072453
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note
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It is conventional to define ξ in terms of the grand canonical distribution function ḡ(r), because it is only in this ensemble that ḡ(r), and thus ξ, is related to the isothermal compressibility through the compressibility equation (Ref. 51).
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58
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85033045590
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x+
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x+.
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59
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85033042763
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The radial distribution functions are all step functions as a result of the design of the idealized system
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The radial distribution functions are all step functions as a result of the design of the idealized system.
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60
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85033055546
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For simplicity in the present discussion we neglect the presence of the average atoms as they do not appear in the partial distribution functions of interest
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For simplicity in the present discussion we neglect the presence of the average atoms as they do not appear in the partial distribution functions of interest.
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61
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85033052421
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note
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lo, or N. This result will be valid given a sufficiently large initial canonical ensemble.
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