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...
Main Authors: | , , , , , |
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Format: | Article |
Language: | English |
Published: |
SpringerOpen
2017-04-01
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Series: | European Physical Journal C: Particles and Fields |
Subjects: | |
Online Access: | http://link.springer.com/article/10.1140/epjc/s10052-017-4820-y |