2d Gauge Theories and Generalized Geometry
arXiv:1407.5439 · doi:10.1007/JHEP08(2014)021
Abstract
We show that in the context of two-dimensional sigma models minimal coupling of an ordinary rigid symmetry Lie algebra leads naturally to the appearance of the "generalized tangent bundle" by means of composite fields. Gauge transformations of the composite fields follow the Courant bracket, closing upon the choice of a Dirac structure (or, more generally, the choide of a "small Dirac-Rinehart sheaf" ), in which the fields as well as the symmetry parameters are to take values. In these new variables, the gauge theory takes the form of a (non-topological) Dirac sigma model, which is applicable in a more general context and proves to be universal in two space-time dimensions: A gauging of of a standard sigma model with Wess-Zumino term exists, \emph{iff} there is a prolongation of the rigid symmetry to a Lie algebroid morphism from the action Lie algebroid into (or the algebraic analogue of the morphism in the case of ). The gauged sigma model results from a pullback by this morphism from the Dirac sigma model, which proves to be universal in two-spacetime dimensions in this sense.
22 pages, 2 figures; To appear in Journal of High Energy Physics
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- Strings in Singular Space-Times and their Universal Gauge Theory
- On the relation of Lie algebroids to constrained systems and their BV/BFV formulation
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