$2+1$ Covariant Lattice Theory and t'Hooft's Formulation

We show that ‘t Hooft’s representation of (2+1)-dimensional gravity in terms of flat polygonal tiles is closely related to a gauge-fixed version of the covariant Hamiltonian lattice theory. ‘t Hooft’s gauge is remarkable in that it leads to a Hamiltonian which is a linear sum of vertex Hamiltonians, each of which is defined modulo $2\pi$. A cyclic Hamiltonian implies that time'' is quantized. However, it turns out that this Hamiltonian is {\it constrained}. If one chooses an internal time and solves this constraint for the physical Hamiltonian’’, the result is not a cyclic function. Even if one quantizes {\it a la Dirac}, the internal time'' observable does not acquire a discrete spectrum. We also show that in Euclidean 3-d lattice gravity, space’’ can be either discrete or continuous depending on the choice of quantization. Finally, we propose a generalization of 't Hooft’s gauge for Hamiltonian lattice formulations of topological gravity dimension 4.