Canonical Quantization of Two Dimensional Gauge Fields
arXiv:hep-lat/9305020 · doi:10.1142/S0217751X94001242
Abstract
gauge fields on a cylindrical spacetime are canonically quantized via two routes revealing almost equivalent but different quantizations. After removing all continuous gauge degrees of freedom, the canonical coordinate (in the Cartan subalgebra $\h$) is quantized. The compact route, as in lattice gauge theory, quantizes the Wilson loop , projecting out gauge invariant wavefunctions on the group manifold . After a Casimir energy related to the curvature of is added to the compact spectrum, it is seen to be a subset of the non-compact spectrum. States of the two quantizations with corresponding energy are shifted relative each other, such that the ground state on , , is the first excited state on $\h$. The ground state does not appear in the character spectrum as its lift is not globally defined on . Implications for lattice gauge theory and the sum over maps representation of two dimensional QCD are discussed.
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