Equivalence between the Lovelock–Cartan action and a constrained gauge theory

Abstract We show that the four-dimensional Lovelock–Cartan action can be derived from a massless gauge theory for the SO(1, 3) group with an additional BRST trivial part. The model is originally composed of a topological sector and a BRST exact piece and has no explicit dependence on the metric, the...

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Bibliographic Details
Main Authors: O. C. Junqueira, A. D. Pereira, G. Sadovski, T. R. S. Santos, R. F. Sobreiro, A. A. Tomaz
Format: Article
Language:English
Published: SpringerOpen 2017-04-01
Series:European Physical Journal C: Particles and Fields
Subjects:
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-017-4820-y