Polytropic dark matter flows illuminate dark energy and accelerated expansion

被引:24
|
作者
Kleidis, K. [1 ]
Spyrou, N. K. [2 ]
机构
[1] Technol Educ Inst Cent Macedonia, Dept Mech Engn, Serres 62124, Greece
[2] Aristotle Univ Thessaloniki, Dept Astron, Thessaloniki 54124, Greece
关键词
dark matter; dark energy; PROBE WMAP OBSERVATIONS; HUBBLE-SPACE-TELESCOPE; GENERALIZED CHAPLYGIN-GAS; HIGH-REDSHIFT SUPERNOVAE; LARGE-SCALE STRUCTURE; BVRI LIGHT CURVES; EQUATION-OF-STATE; IA SUPERNOVAE; OBSERVATIONAL EVIDENCE; CARDASSIAN EXPANSION;
D O I
10.1051/0004-6361/201424402
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Currently, a large amount of data implies that the matter constituents of the cosmological dark sector might be collisional. An attractive feature of such a possibility is that, it can reconcile dark matter (DM) and dark energy (DE) in terms of a single component, accommodated in the context of a polytropic-DM fluid. In fact, polytropic processes in a DM fluid have been most successfully used in modeling dark galactic haloes, thus significantly improving the velocity dispersion profiles of galaxies. Motivated by such results, we explore the time evolution and the dynamical characteristics of a spatially-flat cosmological model, in which, in principle, there is no DE at all. Instead, in this model, the DM itself possesses some sort of fluidlike properties, i.e., the fundamental units of the Universe matter-energy content are the volume elements of a DM fluid, performing polytropic flows. In this case, together with all the other physical characteristics, we also take the energy of this fluid's internal motions into account as a source of the universal gravitational field. This form of energy can compensate for the extra energy, needed to compromise spatial flatness, namely, to justify that, today, the total energy density parameter is exactly unity. The polytropic cosmological model, depends on only one free parameter, the corresponding (polytropic) exponent, Gamma. We find this model particularly interesting, because for Gamma <= 0.541, without the need for either any exotic DE or the cosmological constant, the conventional pressure becomes negative enough so that the Universe accelerates its expansion at cosmological redshifts below a transition value. In fact, several physical reasons, e.g., the cosmological requirement for cold DM (CDM) and a positive velocity-of-sound square, impose further constraints on the value of G, which is eventually settled down to the range -0.089 < Gamma <= 0. This cosmological model does not suffer either from the age problem or from the coincidence problem. At the same time, this model reproduces to high accuracy the distance measurements performed with the aid of the supernovae (SNe) Type Ia standard candles, and most naturally interprets, not only when, but also why the Universe transits from deceleration to acceleration, thus arising as a mighty contestant for a DE model.
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页数:16
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