Non-linear matter power spectrum without screening dynamics modelling in gravity
arXiv:2001.09229 · doi:10.1093/mnras/staa006
Abstract
Halo model is a physically intuitive method for modelling the non-linear power spectrum, especially for the alternatives to the standard CDM models. In this paper, we exam the Sheth-Tormen barrier formula adopted in the previous \texttt{CHAM} method \citep{2018MNRAS.476L..65H}. As an example, we model the ellipsoidal collapse of top-hat dark matter haloes in gravity. A good agreement between Sheth-Tormen formula and our result is achieved. The relative difference in the ellipsoidal collapse barrier is less than or equal to . Furthermore, we verify that, for F4 and F5 cases of Hu-Sawicki gravity, the screening mechanism do not play a crucial role in the non-linear power spectrum modelling up to . We compare two versions of modified gravity modelling, namely with/without screening. We find that by treating the effective Newton constant as constant number () is acceptable. The scale dependence of the gravitational coupling is sub-relevant. The resulting spectra in F4 and F5, are in agreement with the previous \texttt{CHAM} results. The published code is accelerated significantly. Finally, we compare our halo model prediction with N-body simulation. We find that the general spectrum profile agree, qualitatively. However, via the halo model approach, there exists a systematic under-estimation of the matter power spectrum in the co-moving wavenumber range between and . These scales are overlapping with the transition scales from two halo term dominated regimes to those of one halo term dominated.
Accepted in MNRAS
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