Abstract
Application of the critical dynamics to the nucleation process results in a Langevin-type equation for the radius of the nucleus, which is transformed to a Fokker-Planck equation for the distribution function. The time-dependent solution of this equation is shown to be crucially dependent upon the initial conditions. The time lag associated with the establishment of the steady state following a fast quench is exponentially larger than that for a slow quench. Numerical estimates of the time lag are presented.
Original language | English |
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Pages (from-to) | 1496-1505 |
Number of pages | 10 |
Journal | Physical Review A |
Volume | 29 |
Issue number | 3 |
DOIs | |
State | Published - 1984 |