Curved Yang-Mills gauge theories and their recent applications
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Fokko du Cloux
Bâtiment Braconnier
We will study curved Yang-Mills gauge theories, motivated by the infinitesimal gauge theory developed by Alexei Kotov and Thomas Strobl. These gauge theories are based on principal bundles equipped with a Lie group bundle action, in contrast to a Lie group action. In order to define a gauge invariant theory we have to introduce a connection on the structural Lie group bundle, and we impose conditions on its connection 1-form: It has to be a multiplicative form, i.e. closed w.r.t. a certain simplicial differential, and its curvature has to be exact; the connection 1-form is a generalization of the Maurer-Cartan form of the classical gauge theory, while the exactness of its curvature will generalize the role of the Maurer-Cartan equation. For allowing curved connections, while preserving gauge invariance, we will need to generalize the typical definition of the curvature/field strength on the principal bundle, by essentially accounting the curvature on the group bundle. If the connection on the group bundle is flat, the gauge theory is called to be flat and thus (almost) an ordinary gauge theory.