2016
DOI: 10.1088/1475-7516/2016/07/024
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Dynamics of the diffusive DM-DE interaction – Dynamical system approach

Abstract: Abstract. We discuss dynamics of a model of an energy transfer between dark energy (DE) and dark matter (DM). The energy transfer is determined by a non-conservation law resulting from a diffusion of dark matter in an environment of dark energy. The relativistic invariance defines the diffusion in a unique way. The system can contain baryonic matter and radiation which do not interact with the dark sector. We treat the Friedman equation and the conservation laws as a closed dynamical system. The dynamics of… Show more

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Cited by 26 publications
(31 citation statements)
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“…Beyond those approaches, a unification of Dark Energy and Dark Matter using a new measure of integration (the so-called Two Measure Theories) has been formulated [21]- [25]. A diffusive interaction between dark energy and dark matter was introduced in [26]- [32] and was formulated in the context of an action principle based on a generalization of those Two Measures Theories in the context of quintessential scalar fields [27]- [28].…”
Section: Introductionmentioning
confidence: 99%
“…Beyond those approaches, a unification of Dark Energy and Dark Matter using a new measure of integration (the so-called Two Measure Theories) has been formulated [21]- [25]. A diffusive interaction between dark energy and dark matter was introduced in [26]- [32] and was formulated in the context of an action principle based on a generalization of those Two Measures Theories in the context of quintessential scalar fields [27]- [28].…”
Section: Introductionmentioning
confidence: 99%
“…One interesting suggestion was a diffusive exchange of energy between dark energy and dark matter made by Calogero [9,10], Haba et al [11], and Szydlowski and Stachowski [12], with some solution to cosmic problems. The basic notion is that the diffusion equation (or more exactly, the Fokker-Planck equation [13,14], which describes the time evolution of the probability density function of the velocity of a particle under the influence of random forces), implies a non-conserved stress energy tensor T μν , which has some current source j μ :…”
Section: Introductionmentioning
confidence: 99%
“…In order to obtain the results in the complete model we would have to solve (numerically) equations of Section 7. The comparison of density evolution (38) with observations is discussed in [32] and in similar models with the decaying vacuum ( see [34,35] and references cited there). The model allows calculating (and compare with observations) the power spectrum resulting from thermal fluctuations which may go beyond the approximations applied in the warm inflation of [20].…”
Section: Discussionmentioning
confidence: 99%
“…has the meaning of the inverse temperature. The dependence (38) of the temperature of the diffusing system on the scale factor has been derived (for = 0 and arbitrary ) in [31][32][33] for any system with = 1 and the −3 correction (35) to the cosmological term (in eq. (38) = 1) (for timedependent cosmological term see [5,34,35]).…”
Section: A Simplified System Of a Decaying Inflatonmentioning
confidence: 99%