Problems for mond in clusters and the ly α forest

semanticscholar(2001)

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Draft ABSTRACT The observed dynamics of gas and stars on galactic and larger scales cannot be accounted for by self-gravity, indicating that there are large quantities of unseen matter, or that gravity is non-Newtonian in these regimes. Milgrom's MOdified Newtonian Dynamics (MOND) postulates that Newton's laws are modified at very low acceleration, and can account for the rotation curves of galaxies and some other astrophysical observations, without dark matter. Here we apply MOND to two independent physical systems: Lyα absorbers and galaxy clusters. While physically distinct, both are simple hydrodynamical systems with characteristic accelerations in the MOND regime. We find that Lyα absorbers are more dense and about ten times smaller than in Newtonian gravity with dark matter, in disagreement with sizes inferred from quasar pair studies. The mass density of gas in the absorption systems inferred using number counts of the absorption lines is, however, reasonable. In clusters MOND appears to explain the observed (baryonic) mass-temperature relation. However, given observed gas density and enclosed mass profiles and the assumption of hydrostatic equilibrium, MOND predicts radial temperature profiles which disagree badly with observations. We show this explicitly for the Virgo and Abell 2199 clusters, but the results are general, and seem very difficult to avoid. This result strongly disfavors MOND as an alternative to dark matter. Subject headings: cosmology: theory – gravitation – dark matter – galaxies: clusters: general – intergalactic medium – hydrodynamics 1. INTRODUCTION The currently most widely-accepted 'standard model' of cosmology holds that the vast majority of the mass density of the universe is hidden in dark forms. The rotation curves of galaxies and the dynamics of galaxy clusters cannot be accounted for by the gravitation of visible stars and gas, while constraints from primordial nucleosynthesis studies imply that the additional 'dark matter' postulated to remedy this discrepancy must be non-baryonic. On a cosmological level, collisionless (or very weakly collisional) dark matter is required if primordial density perturbations of amplitude ∆ρ/ρ ∼ 10 −5 are to grow quickly enough to form galaxies by the present epoch. Finally, recent deter-minations of the high redshift type Ia supernova Hubble diagram, in tandem with microwave background data implying a flat cosmic geometry, and a large collection of data indicating that clustering matter only contributes ∼ 30% of the critical density, imply that the universe also contains 'dark energy' of a yet more exotic form which causes acceleration in the cosmic …
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