MONTHLY NOTICES OF THE ROYAL ASTRONOMICAL SOCIETY, v.284, no.2, pp.416 - 424
Abstract
During the formation of large-scale structure in the Universe, matter accretes on to high-density peaks. Accreting collisionless dark matter (DM) forms caustics around them, while accreting collisional baryonic matter (BM) forms accretion shocks. The properties of the accreting matter depend upon the power spectrum of the initial perturbations on a given scale as well as the background expansion in a given cosmological model. In this paper, we have calculated the accretion of DM particles in one-dimensional spherical geometry under various cosmological models including the Einstein-de Sitter universe, the open universe with Omega(0) < 1, and the flat universe with Omega(A) = 1 - Omega(0). A density parameter in the range 0.1 less than or equal to Omega(0) less than or equal to 1 has been considered. The initial perturbation characterized by a point mass at the origin has been considered. Since the accretion shock of BM is expected to form close to the first caustic of DM, the properties of the accreting BM are common with those of the DM. Hence, the accretion calculations with DM particles have been used to find the position and velocity of the accretion shock and the cluster mass inside it. The average temperature of BM has been estimated by adopting simplifying assumptions. The velocity of the accreting BM around clusters of a given temperature is lower in a universe with lower Omega(0), but only by up to similar to 24 per cent in the models with 0.1 less than or equal to Omega(0) less than or equal to 1. Thus, it would be difficult to use that quantity to discriminate among the cosmological models. However, the accretion velocity around clusters of a given mass or a given radius depends more sensitively on the cosmological models. It is lower in a universe with lower Omega(0) by up to similar to 41 and similar to 65 per cent, respectively. So, it can provide a better signature of the background expansion for different cosmological models. Although the existence of the caustics and the accretion shocks may not be confirmed by direct X-ray observations, the infalling warm gas of 10(4)-10(5) K upstream of the shocks may be observed as the absorption systems of quasar emission lines. According to this study, the suggestion made by Kang, Ryu & Jones that the large-scale accretion shocks around clusters of galaxies can serve as possible acceleration sites of ultrahigh-energy cosmic rays above 10(18) eV remains plausible in all viable cosmological models