2015
DOI: 10.1103/physrevd.91.024021
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Gauge connection formulations for general relativity

Abstract: We report a new class of $SO(3,\mathbb{C})$ and diffeomorphism invariant formulations for general relativity with either a vanishing or a nonvanishing cosmological constant, which depends functionally on a $SO(3,\mathbb{C})$ gauge connection and a complex-valued 4-form via a holomorphic function of the trace of a symmetric $3\times3$ matrix that is constructed from these variables. We present two members of this class, one of which results from the implementation of a method for obtaining action principles bel… Show more

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Cited by 4 publications
(7 citation statements)
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“…By eliminating auxiliary fields in Plebanski's action, it is possible to derive interesting alternative formulations of general relativity. Such is the case of the CDJ formulation [20,21], the pure connection formulation [25], and the gauge connection formulations of [79]. The aim of this section is to review how these formulations emerge from the Plebanski formulation.…”
mentioning
confidence: 99%
“…By eliminating auxiliary fields in Plebanski's action, it is possible to derive interesting alternative formulations of general relativity. Such is the case of the CDJ formulation [20,21], the pure connection formulation [25], and the gauge connection formulations of [79]. The aim of this section is to review how these formulations emerge from the Plebanski formulation.…”
mentioning
confidence: 99%
“…On the other hand, notice that Plebanski's action emerges from ( 79) when B i is integrated out. Indeed, the variation with respect to B i leads to B i = Σ i , which in turn substituted into (79) gives precisely Plebanski's action (6), thus concluding our procedure. It is important to emphasize that (6) works well for both Λ = 0 and Λ = 0, and that its equivalence with the pure connection action (74) holds whenever X is invertible and Λ = 0.…”
Section: 17mentioning
confidence: 65%
“…where f ′ = df /dTrΨ, the action (76) describes general relativity [79]. In particular, these properties are enjoyed by f = α 1 (2TrΨ + Λ) + α 2 (TrΨ + Λ) 2 if the constants α 1 and α 2 are such that α 1 = 0 and α 1 + α 2 Λ = 0 with Λ = 0 or Λ = 0.…”
Section: Canonical Analysismentioning
confidence: 99%

$BF$ gravity

Celada,
González,
Montesinos
2016
Preprint
Self Cite
“…(iii) In the context of the formulations explored in Ref. [23], the action principle (15) (iv) For λ = 0 and β = 0, the action (1) describes conformally anti-self-dual gravity. In fact, by eliminating the B field and ρ from it, we arrive at the action of Ref.…”
Section: Discussionmentioning
confidence: 99%