2007
DOI: 10.1111/j.1365-2966.2007.12413.x
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Constraining dark energy anisotropic stress

Abstract: We investigate the possibility of using cosmological observations to probe and constrain an imperfect dark energy fluid. We consider a general parametrization of the dark energy component accounting for an equation of state, speed of sound and viscosity. We use present and future data from the cosmic microwave background (CMB) radiation, large-scale structures and Type Ia supernovae. We find that both the speed of sound and viscosity parameters are difficult to nail down with the present cosmological data. Als… Show more

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Cited by 122 publications
(88 citation statements)
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“…Moreover, the growth of cosmic structures are also affected by perturbations of DE when we deal with dynamical DE models with time varying EoS parameter w 1 de ¹ - (Erickson et al 2002;Bean & Doré 2004;Hu & Scranton 2004;Basilakos & Voglis 2007;Mota et al 2007;Ballesteros & Riotto 2008;Basilakos et al 2009aBasilakos et al , 2010Gannouji et al 2010;Sapone & Majerotto 2012;Batista & Pace 2013;Dossett & Ishak 2013;Basse et al 2014;Batista 2014;Nesseris & Sapone 2015;Pace et al 2014aPace et al , 2014bBasilakos 2015;Mehrabi et al 2015aMehrabi et al , 2015bMehrabi et al , 2015cMalekjani et al 2015Malekjani et al , 2017.…”
Section: Introductionmentioning
confidence: 99%
See 1 more Smart Citation
“…Moreover, the growth of cosmic structures are also affected by perturbations of DE when we deal with dynamical DE models with time varying EoS parameter w 1 de ¹ - (Erickson et al 2002;Bean & Doré 2004;Hu & Scranton 2004;Basilakos & Voglis 2007;Mota et al 2007;Ballesteros & Riotto 2008;Basilakos et al 2009aBasilakos et al , 2010Gannouji et al 2010;Sapone & Majerotto 2012;Batista & Pace 2013;Dossett & Ishak 2013;Basse et al 2014;Batista 2014;Nesseris & Sapone 2015;Pace et al 2014aPace et al , 2014bBasilakos 2015;Mehrabi et al 2015aMehrabi et al , 2015bMehrabi et al , 2015cMalekjani et al 2015Malekjani et al , 2017.…”
Section: Introductionmentioning
confidence: 99%
“…In particular, we can set up a more general formalism in which the background expansion data, including SN Ia, BAO, CMB shift parameter, Hubble expansion data, joined with the growth rate data of LSSs in order to put constraints on the parameters of cosmology and DE models (see Cooray et al 2004;Corasaniti et al 2005;Mota et al 2007Mota et al , 2008Basilakos et al 2010;Gannouji et al 2010;Mota et al 2010;Blake et al 2011b;Nesseris et al 2011;Basilakos & Pouri 2012;Chuang et al 2013;Contreras et al 2013;Llinares & Mota 2013;Llinares et al 2014;Li et al 2014;Yang et al 2014;Basilakos 2015;Mehrabi et al 2015aMehrabi et al , 2015bBasilakos 2016;Bonilla Rivera & Farieta 2016;Fay 2016;Malekjani et al 2017).…”
Section: Introductionmentioning
confidence: 99%
“…While a primordial shear decays if it is not sourced, late-time anisotropy appears in many phenomenological models of dark energy [3][4][5][6][7] and is a generic prediction of bigravity models [8] and backreaction [9]. Contrary to the former [10][11][12][13][14], the latter remains weakly constrained by the observation of the cosmic microwave background temperature field; this naturally stimulated analyses based, e.g., on the observation of supernovae [15][16][17][18][19][20][21][22][23][24][25][26][27], or using low-redshift galaxies [28,29].…”
Section: Introductionmentioning
confidence: 99%
“…Moreover, it could be used to distinguish among scalar field theories in which the possible nonminimal coupling occurs only at the perfect fluid matter sector [36][37][38][39]. Such perturbative shear stresses have in general been attempted to be constrained through parameters describing directly the difference of the metric variables [40] and the viscous properties of generalized fluids [41][42][43]. Unfortunately, the perturbative anisotropic stress could escape detection, when its influences are restricted to so large scales that they are only seen through the amplitude of the first few multipoles of the CMB.…”
Section: Introductionmentioning
confidence: 99%