String hamiltonian from generalized YM gauge theory in two dimensions
arXiv:hep-th/0211133 · doi:10.1142/S0217751X04016489
Abstract
Two dimensional SU(N) Yang-Mills theory is known to be equivalent to a string theory, as found by Gross in the large N limit, using the 1/N expansion. Later it was found that even a generalized YM theory leads to a string theory of the Gross type. In the standard YM theory case, Douglas and others found the string hamiltonian describing the propagation and the interactions of states made of strings winding on a cylindrical space-time. We address the problem of finding a similar hamiltonian for the generalized YM theory. As in the standard case we start by writing the theory as a theory of free fermions. Performing a bosonization, we express the hamiltonian in terms of the modes of a bosonic field, that are interpreted as in the standard case as creation and destruction operators for states of strings winding around the cylindrical space-time. The result is similar to the standard hamiltonian, but with new kinds of interaction vertices.
19 pages
References in corpus (9)
- Two Dimensional QCD is a String Theory
- Lectures on 2D Yang-Mills Theory, Equivariant Cohomology and Topological Field Theories
- Two Dimensional QCD as a String Theory
- Twists and Wilson Loops in the String Theory of Two Dimensional QCD
- Large N 2D Yang-Mills Theory and Topological String Theory
- Equivalence of Two Dimensional QCD and the Matrix Model
- The String Theory Approach to Generalized 2D Yang-Mills Theory
- Summing Over Inequivalent Maps in the String Theory Interpretation of Two Dimensional QCD
- On the String Actions for the Generalized Two-dimensional Yang-Mills Theories