  We theoretically predict two new classes of three-dimensional topological
crystalline insulators (TCIs), which have an odd number of unpinned surface
Dirac cones protected by crystal symmetries. The first class is protected by a
single glide plane symmetry; the second class is protected by a composition of
a twofold rotation and time-reversal symmetry. Both classes of TCIs are
characterized by a quantized $\pi$ Berry phase associated with surface states
and a $Z_2$ topological invariant associated with the bulk bands. In the
presence of disorder, these TCI surface states are protected against
localization by the average crystal symmetries, and exhibit critical
conductivity in the universality class of the quantum Hall plateau transition.
These new TCIs exist in time-reversal-breaking systems with or without
spin-orbital coupling, and their material realizations are discussed.
