A symmetry based quantization method of reparametrization invariant sy
stems is described; it will work for all systems that possess complete
sets of perennials whose Lie algebras close and those that generate s
ufficiently large symmetry groups. The construction leads to a quantum
theory including a Hilbert space, a complete system of operator obser
vables, and a unitary time evolution. The method is applied to the 2+1
gravity. The paper is restricted to the metric-torus sector, zero cos
mological constant Lambda and it makes strong use of the so-called hom
ogeneous gauge; the chosen algebra of perennials is that of Martin. Tw
o frequent problems are tackled. First, the Lie algebra of perennials
does not generate a group of symmetries. The notion of group completio
n of a reparametrization invariant system is introduced so that the gr
oup does act; the group completion of the physical phase space of our
model is shown to add only some limit points to it so that the ranges
of observables are not unduly changed. Second, a relatively large numb
er of relations between observables exists; they are transferred to th
e quantum theory by the well-known methods of Kostant and Kirillov. In
this way, a uniqueness of the physical representation of some extensi
on of Martin's algebra is shown. The Hamiltonian is defined by a syste
matic procedure due to Dirac; for the torus sector, the result coincid
es with that by Moncrief. The construction may be extended to higher g
enera and nonzero Lambda of the 2+1 gravity, because some complete set
s of perennials are well-known and there are no obstructions to the cl
osure of the algebra. (C) 1998 American Institute of Physics.