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/content/aip/journal/jcp/132/4/10.1063/1.3299293
1.
1.V. Holten and M. E. H. van Dongen, J. Chem. Phys. 130, 014102 (2009).
http://dx.doi.org/10.1063/1.3054634
2.
2.V. A. Shneidman, Sov. Phys. Tech. Phys. 32, 76 (1987).
3.
3.V. A. Shneidman, Sov. Phys. Tech. Phys. 33, 1338 (1988).
4.
4.Minor scatter of symbols is due to limited accuracy of reading data from the original Fig. 2 of Ref. 1;
4.For a precise recent comparison, see V. Holten, Ph.D. dissertation, Eindhoven University of Technology, 2009.
5.
5.L. Granasy and P. James, J. Chem. Phys. 113, 9810 (2000);
http://dx.doi.org/10.1063/1.1322030
5.See analysis in V. A. Shneidman and E. V. Goldstein, J. Non-Cryst. Solids 351, 1512 (2005).
http://dx.doi.org/10.1016/j.jnoncrysol.2005.03.039
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/content/aip/journal/jcp/132/4/10.1063/1.3299293
2010-01-26
2016-09-30

Abstract

Numerical results obtained by Holten and van Dongen for the transient nucleation problem at large sizes are compared to the matched asymptotic (singular perturbation)solution of the discrete Becker–Döring equation. For not too small times, the agreement is excellent. Comparison also clarifies the structure of the nucleation source in the growth equation and explains some of the observed scaling dependences.

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