Abstract
Following a suggestion due to Bardeen and Pearson, we formulate an effective light-front Hamiltonian for large- N gauge theory in (2 + 1)-dimensions. Two space-time dimensions are continuous and the remaining space dimension is discretised on a lattice. Eguchi-Kawai reduction to a (1 + 1)-dimensional theory takes place. We investigate the string tension and glueball spectrum, comparing with Euclidean Lattice Monte Carlo data.
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