  The Hamiltonian formulation of the teleparallel equivalent of general
relativity (TEGR) is developed from an ordinary second-order Lagrangian, which
is written as a quadratic form of the coefficients of anholonomy of the
orthonormal frames (vielbeins). We analyze the structure of eigenvalues of the
multi-index matrix entering the (linear) relation between canonical velocities
and momenta to obtain the set of primary constraints. The canonical Hamiltonian
is then built with the Moore-Penrose pseudo-inverse of that matrix. The set of
constraints, including the subsequent secondary constraints, completes a first
class algebra. This means that all of them generate gauge transformations. The
gauge freedoms are basically the diffeomorphisms, and the (local) Lorentz
transformations of the vielbein. In particular, the ADM algebra of general
relativity is recovered as a sub-algebra.
