Dissociation reaction of the 1/3$$ \left\langle {\bar{1}101} \right\rangle $$ edge dislocation in α-Al2O3

Abstract

It has been reported that dislocations with 1/3 $$ \left\langle {\bar{1}101} \right\rangle $$ edge component of the Burgers vector are formed in {1 $$ \bar{1} $$ 04}/ $$ \left\langle {11\bar{2}0} \right\rangle $$ low-angle grain boundaries of alumina (α-Al2O3). These dislocations dissociate into two partial dislocations with a stacking fault on the (0001) plane (Tochigi et al. in J Mater Sci 46:4428–4433, 2011). However, the dissociation reaction of these dislocations has not been determined so far. In this study, the structures of the dissociated dislocations and the (0001) stacking fault were investigated by transmission electron microscopy and theoretical calculations. It was revealed that the dissociated dislocations were generated from the 1/3 $$ \left\langle {\bar{1}101} \right\rangle $$ perfect edge dislocation by the reaction of 1/3 $$ \left\langle {\bar{1}101} \right\rangle $$ → 1/18 $$ \left\langle {\bar{4}223} \right\rangle $$ + 1/18 $$ \left\langle {\bar{2}4\bar{2}3} \right\rangle $$ . Furthermore, electron energy loss spectroscopy analysis was performed to examine the atomic/electronic structure of the (0001) stacking fault. In the observed spectra, a chemical shift and intensity decrease were found at the oxygen K-edge. Theoretical spectrum analysis using first-principles calculations revealed that the characteristic features of the spectra are originated from the local atomic configurations of the (0001) stacking fault.