End-of-range (EOR) defects are interstitial type dislocation loops whi
ch nucleate just beneath the crystalline/amorphous (c/a) interface for
med by ion implantation in Si, after the preamorphization of the subst
rate, and during the ramping-up of the anneal. They originate from the
presence of a high supersaturation of ''excess'' Si self-interstitial
atoms located just beneath the c/a interface. Upon annealing, the mea
n radius of the defects increases while their density decreases throug
h the exchange of Si self-interstitial atoms between the loops. The nu
mber of interstitials stored in the loops stays constant. For sufficie
ntly high thermal budgets, when the nucleation is finished, and when t
he local equilibrium between extended and point defects is established
, the coarsening of the EOR defects can be modeled through the Ostwald
ripening theory applied to the dislocation loops geometry. Indeed, an
d as expected from the theory, the square of the mean radius of the lo
op population increases with time while the loop density decreases pro
portional to 1/t. Furthermore, the theoretical function describing the
size distributions perfectly matches the time evolution of the experi
mental stack histograms, for different annealing temperatures. During
the asymptotic steady-state coarsening regime, the activation energy f
or the loop coarsening is 4.4 eV, which is in the range of values give
n in the literature for self-diffusion in Si. Nevertheless, an activat
ion energy of about 1-2 eV is found during the transient period preced
ing the local equilibrium, i.e., in the range of the migration energy
of self-interstitials. The limiting phenomenon for the loop growth app
ears to be diffusion, since it is the hypothesis that leads to the bes
t fit between theory and experiment. An estimate of DiCi has been der
ived from the growth laws of the EOR defects. A value of about 1.8x10(
7) cm(-1) s(-1) at 1000 degrees C is obtained and compares well with t
he values given in the Literature. (C) 1998 American Institute of Phys
ics.