On Baryon Number Non-Conservation in Two-Dimensional O(2N+1) QCD

Details On Baryon Number Non-Conservation in Two-Dimensional O(2N+1) QCD On Baryon Number Non-Conservation in Two-Dimensional O(2N+1) QCD

2009-11-15

arxiv.org/abs/0911.2921v1

Int.J.Mod.Phys.25:1253-1266,2010

Physics

High Energy Physics

High Energy Physics - Theory

22 pages. Accepted for publication in Int. J. Mod. Phys. A

Scientific paper

10.1142/S0217751X10047853

We construct a classical dynamical system whose phase space is a certain infinite-dimensional Grassmannian manifold, and propose that it is equivalent to the large N limit of two-dimensional QCD with an O(2N+1) gauge group. In this theory, we find that baryon number is a topological quantity that is conserved only modulo 2. We also relate this theory to the master field approach to matrix models.

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