2015
DOI: 10.48550/arxiv.1511.08517
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The KLT relations in unimodular gravity

Abstract: With this article, we initiate a systematic study of some of the symmetry properties of unimodular gravity, building on much of the known structure of general relativity, and utilizing the powerful technology developed in that context. In particular, we show, up to four-points and tree-level, that the KLT relations of perturbative gravity hold for tracefree or unimodular gravity.

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Cited by 8 publications
(10 citation statements)
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“…UG and GR are known to be almost identical at the classical level. Besides the equations of motion, this has been seen also in the tree-level amplitudes [25,26]. The question is then whether this persists when loop effects are taken into account.…”
Section: Discussionmentioning
confidence: 94%
“…UG and GR are known to be almost identical at the classical level. Besides the equations of motion, this has been seen also in the tree-level amplitudes [25,26]. The question is then whether this persists when loop effects are taken into account.…”
Section: Discussionmentioning
confidence: 94%
“…Unimodular gravity satisfies the condition (A) as it is equivalent to the Fierz-Pauli theory at the linear level [55]. (B) and (D) are also satisfied, as unimodular gravity shares the 3-point amplitudes with general relativity and its interaction vertices are quadratic in the momenta [57,58]. On the other hand, its propagator behaves as 1/p 2 for large (off-shell) momenta, thus satisfying (C), with m = 4.…”
Section: B Scattering Amplitudes Of Unimodular Gravitymentioning
confidence: 98%
“…The formalism we shall present constitutes a reconstruction method, and we now we shall briefly present the essential features of this reconstruction method. The standard Einstein gravity approach for unimodular gravity [470,472,475,477,[479][480][481][482][483][484][485], is based on the basic assumption that the determinant of the metric is a fixed number, so that the metric satisfies g µν δg µν = 0, which in effect implies that the various components of the metric can be appropriately adjusted, so that the resulting determinant of the metric √ −g is some fixed function of space-time. Hence, it can be assumed, that the metric tensor satisfies the unimodular constraint of Eq.…”
Section: Unimodular Mimetic Gravitymentioning
confidence: 99%