Abstract

Non-commutative gauge theories with a non-constant NC-parameter are investigated. As a novel approach, we propose that such theories should admit an underlying L∞ algebra, that governs not only the action of the symmetries but also the dynamics of the theory. Our approach is well motivated from string theory. We recall that such field theories arise in the context of branes in WZW models and briefly comment on its appearance for integrable deformations of AdS5 sigma models. For the SU(2) WZW model, we show that the earlier proposed matrix valued gauge theory on the fuzzy 2-sphere can be bootstrapped via an L∞ algebra. We then apply this approach to the construction of non-commutative Chern-Simons and Yang-Mills theories on flat and curved backgrounds with non-constant NC-structure. More concretely, up to the second order, we demonstrate how derivative and curvature corrections to the equations of motion can be bootstrapped in an algebraic way from the L∞ algebra. The appearance of a non-trivial A∞ algebra is discussed, as well.

Highlights

  • Using techniques from conformal field theory, for the SU(2) WZW model it was shown that this theory is a non-commutative matrix valued gauge theory on the fuzzy 2-sphere

  • Non-commutative gauge theories with a non-constant NC-parameter are investigated. We propose that such theories should admit an underlying L∞ algebra, that governs the action of the symmetries and the dynamics of the theory

  • E.g. for bosonic closed string field theory, both the action of symmetries on the string field and their string equations of motion were governed by an L∞ algebra

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Summary

Preliminaries

For self-consistency, we introduce some of the salient features of known NC gauge theories and the formal definitions of L∞ and A∞ algebras. We analyze the NC gauge theory based on the Moyal-Weyl star product with respect to an underlying L∞ algebra

Non-commutative gauge theories
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NC gauge theories arising in string theory
D-Branes in WZW models
Non-constant Θ via integrable deformations
An issue for non-constant Θ
Πijk 3
NC Chern-Simons theory
NC Yang-Mills theory
Conclusions
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Full Text
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