2018
DOI: 10.1088/1475-7516/2018/01/044
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Dark energy survivals in massive gravity after GW170817: SO(3) invariant

Abstract: The recent detection of the gravitational wave signal GW170817 together with an electromagnetic counterpart GRB 170817A from the merger of two neutron stars puts a stringent bound on the tensor propagation speed. This constraint can be automatically satisfied in the framework of massive gravity. In this work we consider a general SO(3)-invariant massive gravity with five propagating degrees of freedom and derive the conditions for the absence of ghosts and Laplacian instabilities in the presence of a matter pe… Show more

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Cited by 30 publications
(28 citation statements)
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“…SM is funded by the Imperial College President's Fellowship. ories of gravity-other models of dark energy, such as vector-tensor gravity or scalar-vector-tensor gravity, have also seen their parameter space remarkably affected (see however [13,14,44] for models that survive the bound). Lorentz-violating theories have also been profoundly constrained [45][46][47], although we shall focus on theories which are fundamentally LI here.…”
Section: Acknowledgmentsmentioning
confidence: 99%
See 1 more Smart Citation
“…SM is funded by the Imperial College President's Fellowship. ories of gravity-other models of dark energy, such as vector-tensor gravity or scalar-vector-tensor gravity, have also seen their parameter space remarkably affected (see however [13,14,44] for models that survive the bound). Lorentz-violating theories have also been profoundly constrained [45][46][47], although we shall focus on theories which are fundamentally LI here.…”
Section: Acknowledgmentsmentioning
confidence: 99%
“…Last year, the first detection of GWs from a neutron star merger (GW170817), some 10 15 light seconds away, which arrived within one second of an optical counterpart (GRB170817A), allowed us to constrain the GW speed with remarkable precision [2-4]with c T the GW phase velocity and c γ the speed of light.Such a constraint has had far-reaching consequences for models of dark energy. Within the context of the Effective Field Theory (EFT) for dark energy [5], it was rapidly pointed out that (1) was sufficient to suppress the EFT operators that predict non-luminal gravitational propagation [6][7][8][9][10][11][12][13][14]. In particular, within the framework of scalar-tensor theories of gravity, Horndeski [15] has played a major part in the past decade as a consistent ghost-free EFT in which the scalar degree of freedom could play the role of dark energy.…”
mentioning
confidence: 99%
“…GW170817 placed constraints on the properties of the progenitor of the binary compact object GW170817 [28], and the GW background from compact binaries [29]. Moreover, GW170817 and GRB 170817A constrained the speed of gravity, the equivalence principle and Lorentz invariance [10], consequently constraining to a large degree gravity theories designed to explain the accelerated expansion of the Universe without dark energy [30][31][32][33][34][35][36][37] (see also [38,39] for earlier work). Furthermore, GW170817 furnished the first ever "standard siren" [40] measurement of the Hubble constant [19].…”
Section: Introductionmentioning
confidence: 99%
“…Several high-precision large-scale structure surveys are planned to come into operation in the very near future, and therefore most attempts so far have focused on studying the cosmological implications of such theories in a hope that the future cosmological surveys will be sufficiently sensitive to judge against or for many of these theories. Notably, however, the recent detection of the GWs originating from a pair of merging neutron stars and the simultaneous detection of their electromagnetic counterpart, events GW170817 [81] and GRB 170817A [82], have proven to be able to provide us with an immense amount of knowledge about the landscape of the possible theories of gravity (mainly) through the strong bounds that they have placed on the speed of GWs [83][84][85][86][87][88][89][90][91][92][93][94][95][96][97][98][99][100] (see also Refs. [101][102][103][104][105] for discussions on the consequences of such strong bounds for classes of modified theories of gravity prior to the actual observations).…”
Section: Introductionmentioning
confidence: 99%