Chern-Simons-Witten Theory as a Topological Fermi Liquid

We reinterpret U (N) Chern-Simons-Witten theory quantized on a torus as a free fermion system. Its Hilbert space and some observables are simply related to those of group quantum mechanics, even at finite N and k. Its large N limit can be described using techniques developed for matrix quantum mechanics and two-dimensional Yang-Mills theory. We discuss the bosonization of this theory, which for YM₂ gave a precise interpretation of Wilson loop operators in terms of string creation and annihilation operators, and examine its consequences for a string interpretation here. The formalism seems entirely adequate for the leading large N results and in a sense can be thought of as a `classical string field theory'. In considering subleading orders in 1/N, we identify some major differences between CSW and YM₂, which must be dealt with to find a CSW gauge string interpretation. Although these particular differences are probably not relevant for `QCD string, ' they do illustrate some of the issues there, and we comment on this. We also propose an approach to dealing with large N transitions.