2012
DOI: 10.1103/physrevd.85.084002
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Spatially covariant theories of a transverse, traceless graviton: Formalism

Abstract: General relativity is a generally covariant, locally Lorentz covariant theory of two transverse, traceless graviton degrees of freedom. According to a theorem of Hojman, Kuchař, and Teitelboim, modifications of general relativity must either introduce new degrees of freedom or violate the principle of local Lorentz covariance. In this paper, we explore modifications of general relativity that retain the same graviton degrees of freedom, and therefore explicitly break Lorentz covariance. Motivated by cosmology,… Show more

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Cited by 27 publications
(51 citation statements)
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“…We have used a battery of techniques in order to gain an intuition of the physical meaning of the existence of these theories. Our main conclusion is that these results strengthen the view that general relativity is a unique theory that is not easily deformed (which is compatible with previous partial analyses [49,50]). This claim follows from a combination of results:…”
Section: Discussionsupporting
confidence: 90%
“…We have used a battery of techniques in order to gain an intuition of the physical meaning of the existence of these theories. Our main conclusion is that these results strengthen the view that general relativity is a unique theory that is not easily deformed (which is compatible with previous partial analyses [49,50]). This claim follows from a combination of results:…”
Section: Discussionsupporting
confidence: 90%
“…This is computed at the linear level in appendix A and the result, in equation (A. 45), shows that the two brackets are not weakly zero. Hence, none of the constraintsR 0 , C or C (2) is first class.…”
Section: First Class Constraints In Bimetric Theorymentioning
confidence: 97%
“…Remarkably some of these restrictions survive under a weaker set of assumptions. For example, without assuming Lorentz invariance (while maintaining space diffs), demanding ghost-freedom or more precisely only 2 propagating modes, one is led inevitably back to the Einstein-Hilbert action [9,10].…”
mentioning
confidence: 99%