Challenges for scaling cosmologies

A cosmological model that aims at solving the coincidence problem should show that dark energy and dark matter follow the same scaling solution from some time onward. At the same time, the model should contain a sufficiently long matter-dominated epoch that takes place before acceleration in order t...

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Hauptverfasser: Amendola, Luca (VerfasserIn) , Quartin, Miguel (VerfasserIn)
Dokumenttyp: Article (Journal)
Sprache:Englisch
Veröffentlicht: 24 July 2006
In: Physical review. D, Particles, fields, gravitation, and cosmology
Year: 2006, Jahrgang: 74, Heft: 2, Pages: 023525
ISSN:1550-2368
DOI:10.1103/PhysRevD.74.023525
Online-Zugang:Verlag, Volltext: http://dx.doi.org/10.1103/PhysRevD.74.023525
Verlag, Volltext: https://link.aps.org/doi/10.1103/PhysRevD.74.023525
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Verfasserangaben:Luca Amendola, Miguel Quartin, Shinji Tsujikawa, and Ioav Waga

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520 |a A cosmological model that aims at solving the coincidence problem should show that dark energy and dark matter follow the same scaling solution from some time onward. At the same time, the model should contain a sufficiently long matter-dominated epoch that takes place before acceleration in order to guarantee a decelerated epoch and structure formation. So a successful cosmological model requires the occurrence of a sequence of epochs, namely, a radiation era, a matter-dominated era, and a final accelerated scaling attractor with Ωφ≃0.7. In this paper we derive the generic form of a scalar-field Lagrangian that possesses scaling solutions in the case where the coupling Q between dark energy and dark matter is a free function of the field φ. We then show, rather surprisingly, that the aforementioned sequence of epochs cannot occur for a vast class of generalized coupled scalar-field Lagrangians that includes, to our knowledge, all scaling models in the current literature. 
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