English

The kinematic Sunyaev-Zel'dovich effect of the large-scale structure (II): the effect of modified gravity

Cosmology and Nongalactic Astrophysics 2018-09-05 v1

Abstract

The key to understand the nature of dark energy relies in our ability to probe the distant Universe. In this framework, the recent detection of the kinematic Sunyaev-Zel'dovich (kSZ) effect signature in the cosmic microwave background obtained with the South Pole Telescope (SPT) is extremely useful since this observable is sensitive to the high-redshift diffuse plasma. We analyse a set of cosmological hydrodynamical simulation with 4 different realisations of a Hu & Sawicki f(R)f(R) gravity model, parametrised by the values of fR,0=(0,106,105,104)\overline{f}_{\rm R,0}=(0,-10^{-6},-10^{-5},-10^{-4}), to compute the properties of the kSZ effect due to the ionized Universe and how they depend on fR,0\overline{f}_{\rm R,0} and on the redshift of reionization, zrez_{\rm re}. In the standard General Relativity limit (fR,0\overline{f}_{\rm R,0}=0) we obtain an amplitude of the kSZ power spectrum of D3000kSZ=4.1\mathcal{D}^{\rm kSZ}_{3000}=4.1\,μ\muK2^2 (zrez_{\rm re}=8.8), close to the +1σ+1\sigma limit of the D3000kSZ=(2.9±1.3)\mathcal{D}^{\rm kSZ}_{3000}=(2.9\pm1.3)\,μ\muK2^2 measurement by SPT. This corresponds to an upper limit on the kSZ contribute from patchy reionization of D3000kSZ,patchy<0.9\mathcal{D}^{\rm kSZ,patchy}_{3000}<0.9\,μ\muK2^2 (95 per cent confidence level). Modified gravity boosts the kSZ signal by about 3, 12 and 50 per cent for fR,0=(106,105,104)\overline{f}_{\rm R,0}=(-10^{-6},-10^{-5},-10^{-4}), respectively, with almost no dependence on the angular scale. This means that with modified gravity the limits on patchy reionization shrink significantly: for fR,0=105\overline{f}_{\rm R,0}=-10^{-5} we obtain D3000kSZ,patchy<0.4\mathcal{D}^{\rm kSZ,patchy}_{3000}<0.4\,μ\muK2^2. Finally, we provide an analytical formula for the scaling of the kSZ power spectrum with zrez_{\rm re} and fR,0\overline{f}_{\rm R,0} at different multipoles: at =3000\ell=3000 we obtain D3000kSZzre0.24(1+fR,0)41\mathcal{D}^{\rm kSZ}_{3000}\propto z_{\rm re}^{0.24}\left(1+\sqrt{\left|\overline{f}_{\rm R,0}\right|}\right)^{41}.

Keywords

Cite

@article{arxiv.1805.11607,
  title  = {The kinematic Sunyaev-Zel'dovich effect of the large-scale structure (II): the effect of modified gravity},
  author = {M. Roncarelli and M. Baldi and F. Villaescusa-Navarro},
  journal= {arXiv preprint arXiv:1805.11607},
  year   = {2018}
}

Comments

11 pages, 5 figures, 2 tables