  We propose a stochastic counterpart of the classical
Kolmogorov-Johnson-Mehl-Avrami (KJMA) model to describe the
nucleation-and-growth phenomena of a stable phase (S-phase). We report that for
growth velocity of S-phase $v=s(t)/t$ where $s(t)$ is the mean value of the
interval size $x$ of metastable phase (M-phase) and for $v=x/\tau(x)$ where
$\tau(x)$ is the mean nucleation time, the system exhibits a power law decay of
M-phase. We also find that the resulting structure exhibits self-similarity and
can be best described as a fractal. Interestingly, the fractal dimension $d_f$
helps generalising the exponent $(1+d_f)$ of the power-law decay. However, when
either $v=v_0$ (constant) or $v=\sigma/t$ ($\sigma$ is a constant) the decay is
exponential and it is accompanied by the violation of scaling.
