2011
DOI: 10.1103/physrevd.84.101502
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U(1) symmetry and elimination of spin-0 gravitons in Horava-Lifshitz gravity without the projectability condition

Abstract: In this paper, we show that the spin-0 gravitons appearing in Horava-Lifshitz gravity without the projectability condition can be eliminated by extending the gauge symmetries of the foliationpreserving diffeomorphisms to include a local U(1) symmetry. As a result, the problems of stability, ghost and different speeds in the gravitational sector are automatically resolved. In addition, with the detailed balance condition softly breaking, the number of independent coupling constants can be significantly reduced … Show more

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Cited by 70 publications
(67 citation statements)
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“…At linear perturbations around the Minkowski background it is known that the nonprojectable U (1) extension has a scalar graviton for a generic choice of coupling constants [16]. On the other hand, if one of the parameters in the IR action (which is denoted as η 2 in the present paper) is set to zero, then linear perturbations in the theory do not contain the scalar graviton [14].…”
Section: Introductionmentioning
confidence: 92%
See 1 more Smart Citation
“…At linear perturbations around the Minkowski background it is known that the nonprojectable U (1) extension has a scalar graviton for a generic choice of coupling constants [16]. On the other hand, if one of the parameters in the IR action (which is denoted as η 2 in the present paper) is set to zero, then linear perturbations in the theory do not contain the scalar graviton [14].…”
Section: Introductionmentioning
confidence: 92%
“…While the original theory with the U (1) symmetry is projectable, it is possible to extend it to a nonprojectable theory [14,15]. At linear perturbations around the Minkowski background it is known that the nonprojectable U (1) extension has a scalar graviton for a generic choice of coupling constants [16].…”
Section: Introductionmentioning
confidence: 99%
“…]. These works were further generalized to the case corresponding to absence of the projectability condition [222]. In both cases (with and without the projectability condition), the spin-0 gravitons are eliminated (due to the U (1) symmetry) and all the problems related to them are then resolved.…”
Section: Hořava-lifshitz Gravitymentioning
confidence: 99%
“…Relative to HLG without the projectability conditions, imposing the detailed balance conditions significantly reduces the number of independent coupling constants [7]. Furthermore, when implementing HLG with and without the projectability conditions in a local U(1) symmetry to the cosmology, it was found that the Friedmann-Lemaitre-Robertson-Walker (FLRW) Universe becomes flat [8,12].…”
Section: Introductionmentioning
confidence: 99%
“…In HLG without the projectability conditions [7,8] and with the projectability conditions [9,10], the spin-0 gravitons could be eliminated though implementing a local U(1) symmetry [11], where various problems concerning instability, strong coupling and different speeds in the gravitational sector are conjectured to be solved [7]. Relative to HLG without the projectability conditions, imposing the detailed balance conditions significantly reduces the number of independent coupling constants [7].…”
Section: Introductionmentioning
confidence: 99%