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Running coupling: does the coupling between dark energy and dark matter change sign during the cosmological evolution?
Running coupling: does the coupling between dark energy and dark matter change sign during the cosmological evolution?
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Running coupling: does the coupling between dark energy and dark matter change sign during the cosmological evolution?
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Running coupling: does the coupling between dark energy and dark matter change sign during the cosmological evolution?
Running coupling: does the coupling between dark energy and dark matter change sign during the cosmological evolution?
Journal Article

Running coupling: does the coupling between dark energy and dark matter change sign during the cosmological evolution?

2011
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Overview
In this paper we put forward a running coupling scenario for describing the interaction between dark energy and dark matter. The dark sector interaction in our scenario is free of the assumption that the interaction term Q is proportional to the Hubble expansion rate and the energy densities of dark sectors. We only use a time-variable coupling b ( a ) (with a the scale factor of the universe) to characterize the interaction Q . We propose a parametrization form for the running coupling b ( a )= b 0 a + b e (1− a ) in which the early-time coupling is given by a constant b e , while today the coupling is given by another constant, b 0 . For investigating the feature of the running coupling, we employ three dark energy models, namely, the cosmological constant model ( w =−1), the constant w model ( w = w 0 ), and the time-dependent w model ( w ( a )= w 0 + w 1 (1− a )). We constrain the models with the current observational data, including the type Ia supernova, the baryon acoustic oscillation, the cosmic microwave background, the Hubble expansion rate, and the X-ray gas mass fraction data. The fitting results indicate that a time-varying vacuum scenario is favored, in which the coupling b ( z ) crosses the noninteracting line ( b =0) during the cosmological evolution and the sign changes from negative to positive. The crossing of the noninteracting line happens at around z =0.2–0.3, and the crossing behavior is favored at about 1 σ confidence level. Our work implies that we should pay more attention to the time-varying vacuum model and seriously consider the phenomenological construction of a sign-changeable or oscillatory interaction between dark sectors.