First Reduce or First Quantize? A Lagrangian Approach and Application to Coset Spaces

TL;DR

This paper compares two quantization methods for constrained Hamiltonian systems, reveals ambiguities in Dirac's approach, and applies the formalism to quantize on coset spaces like spheres, ensuring consistency and equivalence.

Contribution

It introduces a Lagrangian approach to compare reduction and Dirac quantization, revealing ambiguities and applying the method to coset spaces with consistent results.

Findings

Revealed ambiguities in Dirac quantization.

Established relation between propagators in different formalisms.

Successfully quantized on coset spaces like S^2 with consistent results.

Abstract

A Lagrangian treatment of the quantization of first class Hamiltonian systems with constraints and Hamiltonian linear and quadratic in the momenta respectively is performed. The ``first reduce and then quantize'' and the ``first quantize and then reduce'' (Dirac's) methods are compared. A new source of ambiguities in this latter approach is revealed and its relevance on issues concerning self-consistency and equivalence with the ``first reduce'' method is emphasized. One of our main results is the relation between the propagator obtained {\it \`a la Dirac} and the propagator in the full space, eq. (5.25).As an application of the formalism developed, quantization on coset spaces of compact Lie groups is presented. In this case it is shown that a natural selection of a Dirac quantization allows for full self-consistency and equivalence. Finally, the specific case of the propagator on a two-dimensional sphere $S^2$ viewed as the coset space $SU(2)/U(1)$ is worked out.