41 research outputs found

    Euclid preparation. XV. Forecasting cosmological constraints for the Euclid and CMB joint analysis

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    Euclid: Constraining linearly scale-independent modifications of gravity with the spectroscopic and photometric primary probes

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    International audienceThe future Euclid space satellite mission will offer an invaluable opportunity to constrain modifications to general relativity at cosmic scales. We focus on modified gravity models characterised, at linear scales, by a scale-independent growth of perturbations while featuring different testable types of derivative screening mechanisms at smaller nonlinear scales. We consider 3 specific models, namely Jordan-Brans-Dicke (JBD), the normal branch of Dvali-Gabadadze-Porrati (nDGP) gravity and kk-mouflage (KM) gravity. We provide forecasts from spectroscopic and photometric primary probes by Euclid on the cosmological parameters and the extra parameters of the models, respectively, ωBD\omega_{\rm BD}, Ωrc\Omega_{\rm rc} and ϵ2,0\epsilon_{2,0}, which quantify the deviations from general relativity. This analysis will improve our knowledge of the cosmology of these modified gravity models. The forecasts analysis employs the Fisher matrix method applied to weak lensing (WL); photometric galaxy clustering (GCph_{ph}); spectroscopic galaxy clustering (GCsp_{sp}) and the cross-correlation (XC) between GCph_{ph} and WL. For the Euclid survey specifications we define three scenarios, characterised by different cuts in \ell and kk, to assess the constraining power of nonlinear scales. For each model we consider two fiducial values for the corresponding model parameter. In an optimistic setting at 68.3% confidence interval, with Euclid alone we find the following percentage relative errors: for log10ωBD\log_{10}{\omega_{\rm BD}}, with a fiducial value of ωBD=800\omega_{\rm BD}=800, 35% using GCsp_{sp} alone, 3.6% using GCph_{ph}+WL+XC and 3.3% using GCph_{ph}+WL+XC+GCsp_{sp}; for log10Ωrc\log_{10}{\Omega_{\rm rc}}, with a fiducial value of Ωrc=0.25\Omega_{\rm rc}=0.25, we find respectively 90%, 20% and 17%; finally, for ϵ2,0=0.04\epsilon_{2,0}=-0.04 respectively 5%, 0.15% and 0.14%. (abridged

    Euclid: Constraining linearly scale-independent modifications of gravity with the spectroscopic and photometric primary probes

    No full text
    International audienceThe future Euclid space satellite mission will offer an invaluable opportunity to constrain modifications to general relativity at cosmic scales. We focus on modified gravity models characterised, at linear scales, by a scale-independent growth of perturbations while featuring different testable types of derivative screening mechanisms at smaller nonlinear scales. We consider 3 specific models, namely Jordan-Brans-Dicke (JBD), the normal branch of Dvali-Gabadadze-Porrati (nDGP) gravity and kk-mouflage (KM) gravity. We provide forecasts from spectroscopic and photometric primary probes by Euclid on the cosmological parameters and the extra parameters of the models, respectively, ωBD\omega_{\rm BD}, Ωrc\Omega_{\rm rc} and ϵ2,0\epsilon_{2,0}, which quantify the deviations from general relativity. This analysis will improve our knowledge of the cosmology of these modified gravity models. The forecasts analysis employs the Fisher matrix method applied to weak lensing (WL); photometric galaxy clustering (GCph_{ph}); spectroscopic galaxy clustering (GCsp_{sp}) and the cross-correlation (XC) between GCph_{ph} and WL. For the Euclid survey specifications we define three scenarios, characterised by different cuts in \ell and kk, to assess the constraining power of nonlinear scales. For each model we consider two fiducial values for the corresponding model parameter. In an optimistic setting at 68.3% confidence interval, with Euclid alone we find the following percentage relative errors: for log10ωBD\log_{10}{\omega_{\rm BD}}, with a fiducial value of ωBD=800\omega_{\rm BD}=800, 35% using GCsp_{sp} alone, 3.6% using GCph_{ph}+WL+XC and 3.3% using GCph_{ph}+WL+XC+GCsp_{sp}; for log10Ωrc\log_{10}{\Omega_{\rm rc}}, with a fiducial value of Ωrc=0.25\Omega_{\rm rc}=0.25, we find respectively 90%, 20% and 17%; finally, for ϵ2,0=0.04\epsilon_{2,0}=-0.04 respectively 5%, 0.15% and 0.14%. (abridged

    Euclid: Constraining linearly scale-independent modifications of gravity with the spectroscopic and photometric primary probes

    No full text
    The future Euclid space satellite mission will offer an invaluable opportunity to constrain modifications to general relativity at cosmic scales. We focus on modified gravity models characterised, at linear scales, by a scale-independent growth of perturbations while featuring different testable types of derivative screening mechanisms at smaller nonlinear scales. We consider 3 specific models, namely Jordan-Brans-Dicke (JBD), the normal branch of Dvali-Gabadadze-Porrati (nDGP) gravity and kk-mouflage (KM) gravity. We provide forecasts from spectroscopic and photometric primary probes by Euclid on the cosmological parameters and the extra parameters of the models, respectively, ωBD\omega_{\rm BD}, Ωrc\Omega_{\rm rc} and ϵ2,0\epsilon_{2,0}, which quantify the deviations from general relativity. This analysis will improve our knowledge of the cosmology of these modified gravity models. The forecasts analysis employs the Fisher matrix method applied to weak lensing (WL); photometric galaxy clustering (GCph_{ph}); spectroscopic galaxy clustering (GCsp_{sp}) and the cross-correlation (XC) between GCph_{ph} and WL. For the Euclid survey specifications we define three scenarios, characterised by different cuts in \ell and kk, to assess the constraining power of nonlinear scales. For each model we consider two fiducial values for the corresponding model parameter. In an optimistic setting at 68.3% confidence interval, with Euclid alone we find the following percentage relative errors: for log10ωBD\log_{10}{\omega_{\rm BD}}, with a fiducial value of ωBD=800\omega_{\rm BD}=800, 35% using GCsp_{sp} alone, 3.6% using GCph_{ph}+WL+XC and 3.3% using GCph_{ph}+WL+XC+GCsp_{sp}; for log10Ωrc\log_{10}{\Omega_{\rm rc}}, with a fiducial value of Ωrc=0.25\Omega_{\rm rc}=0.25, we find respectively 90%, 20% and 17%; finally, for ϵ2,0=0.04\epsilon_{2,0}=-0.04 respectively 5%, 0.15% and 0.14%. (abridged
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