Brittle fracture usually proceeds at crack driving forces which are larger
than those needed to create the new fracture surfaces. This surplus can lea
d to faster crack propagation or to the onset of additional dissipation mec
hanisms. Dynamic fracture experiments on silicon single crystals reported h
ere show several distinct transitions between different dissipation mechnni
sms. Cleavage fracture is followed by the propagation of a faceted crack fr
ont, which is finally followed by a path instability and the propagation of
multiple cracks. The fracture surface qualitatively corresponds to the mir
ror, mist, and hackle morphology of amorphous materials. However, the corre
sponding fracture mechanisms, which remain largely unknown in the amorphous
materials, can clearly be identified here.