Abstract
Li, Kadiri and Horstemeyer Citation[1] recently studied
twinning in titanium by atomic-scale computer simulation and proposed a new mechanism in which elementary twinning dislocations (TDs) are nucleated and glide in an extended fashion on adjacent planes. In this comment, we argue that the interpretation of the simulations is in error for several reasons. First, the Burgers vector of the TDs seen in the simulations was not determined correctly. Second, these TDs do not produce the
twin mode known to occur in titanium. Third, the experimentally observed mode occurs under c-axis compression, whereas the motion of the twin boundary in Citation[1] was in response to c-axis tension. The former mode cannot be simulated with the MD model used in Citation[1]. Fourth, the temperature dependence of
twinning found experimentally was misunderstood in Citation[1]. We conclude that the TD responsible for this deformation mode is the one long-established by classical twinning theory and studied at the atomic level by computer simulations performed more than 20 years ago.
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Notes
1. This mapping assumes that the interface structures in Figure 3 are identical on either side of the defect. In fact, the lower crystal appears to be rigidly displaced leftwards slightly away from the mirror reflection position on the left-hand side, and displaced rightwards on the right-hand side. Such a change in the state of rigid-body displacement, if real, would modify the magnitude of b of the disconnection [6].