Abstract

Photoelectron spectroscopy (PES) can be profitably employed for studying three-dimensional phase-transition kinetics as long as the problem of finite escape depth and the presence of the surface is correctly taken into account. A general solution of this problem is presented for transformations following the Johnson-Mehl-Avrami-Kolmogorov kinetics. The cases of simultaneous and constant nucleation rates are discussed. We found that the simple relationship between the PES signal I(t) and the untransformed phase X(t): I(t)=I(0)X(t${)}^{1\mathrm{/}2}$ is an excellent approximation for the simultaneous nucleation and turns out to be quite good for the constant nucleation case.

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