Table 1.
Graphite | hBN | MoSe2 | ||||||
---|---|---|---|---|---|---|---|---|
Direction of twin boundary | ac | zz | ac | zz | ac | zz | ||
Slip direction | zz | ac | zz | ac | zz | ac | ||
L slip | α | α / √ 3 | 2α / √ 3 | 3α / √ 3 | α | 3α / √ 3 | α | 3α / √ 3 |
c (nm) | 0.67 | 0.67 | 0.67 | 0.67 | 0.67 | 0.67 | 1.23 | 1.23 |
a (nm) | 0.25 | 0.25 | 0.25 | 0.25 | 0.25 | 0.25 | 0.33 | 0.33 |
Lslip (nm) | 0.25 | 0.14 | 0.29 | 0.43 | 0.25 | 0.43 | 0.33 | 0.56 |
θt(°) | 40.3 | 23.9 | 46.0 | 64.9 | 41.2 | 65.9 | 30.0 | 48.6 |
Higher order twin zz angles in graphite (2α/√3 and 3α/√3) are likely to be less favourable due to the ease of splitting of such basal dislocations into separate partial dislocations with lower energy