  Nematic ordering, where the spins globally align along a spontaneously chosen
axis irrespective of direction, occurs in spin-glass systems of classical
Heisenberg spins in d=3. In this system where the nearest-neighbor interactions
are quenched randomly ferromagnetic or antiferromagnetic, instead of the
locally randomly ordered spin-glass phase, the system orders globally as a
nematic phase. The system is solved exactly on a hierarchical lattice and,
equivalently, Migdal-Kadanoff approximately on a cubic lattice. The global
phase diagram is calculated, exhibiting this nematic phase, and ferromagnetic,
antiferromagnetic, disordered phases. The nematic phase of the classical
Heisenberg spin-glass system is also found in other dimensions d>2: We
calculate nematic transition temperatures in 24 dimensions in 2<d=<4.
