Model-independent reconstruction of the linear anisotropic stress [eta]

In this work, we use recent data on the Hubble expansion rate H ( z ), the quantity f σ 8 ( z ) from redshift space distortions and the statistic E g from clustering and lensing observables to constrain in a model-independent way the linear anisotropic stress parameter η. This estimate is free of as...

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Hauptverfasser: Pinho, Ana Marta (VerfasserIn) , Casas, Santiago (VerfasserIn) , Amendola, Luca (VerfasserIn)
Dokumenttyp: Article (Journal)
Sprache:Englisch
Veröffentlicht: 19 November 2018
In: Journal of cosmology and astroparticle physics
Year: 2018, Heft: 11
ISSN:1475-7516
DOI:10.1088/1475-7516/2018/11/027
Online-Zugang:Verlag, Volltext: http://dx.doi.org/10.1088/1475-7516/2018/11/027
Verlag, Volltext: http://stacks.iop.org/1475-7516/2018/i=11/a=027
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Verfasserangaben:Ana Marta Pinho, Santiago Casas and Luca Amendola

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520 |a In this work, we use recent data on the Hubble expansion rate H ( z ), the quantity f σ 8 ( z ) from redshift space distortions and the statistic E g from clustering and lensing observables to constrain in a model-independent way the linear anisotropic stress parameter η. This estimate is free of assumptions about initial conditions, bias, the abundance of dark matter and the background expansion. We denote this observable estimator as η obs . If η obs turns out to be different from unity, it would imply either a modification of gravity or a non-perfect fluid form of dark energy clustering at sub-horizon scales. Using three different methods to reconstruct the underlying model from data, we report the value of η obs at three redshift values, z =0.29, 0.58, 0.86. Using the method of polynomial regression, we find η obs =0.57±1.05, η obs =0.48±0.96, and η obs =−0.11±3.21, respectively. Assuming a constant η obs in this range, we find η obs =0.49±0.69. We consider this method as our fiducial result, for reasons clarified in the text. The other two methods give for a constant anisotropic stress η obs =0.15±0.27 (binning) and η obs =0.53 ± 0.19 (Gaussian Process). We find that all three estimates are compatible with each other within their 1σ error bars. While the polynomial regression method is compatible with standard gravity, the other two methods are in tension with it. 
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