Can the clustered dark matter and the smooth dark energy arise from the same scalar field?

dc.contributor.authorPadmanabhan, T.
dc.contributor.authorChoudhury, T. Roy
dc.date.accessioned2012-03-12T09:20:39Z
dc.date.available2012-03-12T09:20:39Z
dc.date.issued2011-07-06
dc.description.abstractCosmological observations suggest the existence of two different kinds of energy densities domi- nating at small (< ∼ 500 Mpc) and large (> ∼ 1000 Mpc) scales. The dark matter component, which dominates at small scales, contributes Ωm ≈ 0.35 and has an equation of state p = 0, while the dark energy component, which dominates at large scales, contributes ΩV ≈ 0.65 and has an equation of state p ≃ −ρ. It is usual to postulate weakly interacting massive particles (WIMPs) for the first component and some form of scalar field or cosmological constant for the second component. We explore the possibility of a scalar field with a Lagrangian L = −V (φ) p1 − ∂iφ∂iφ acting as both clustered dark matter and smoother dark energy and having a scale-dependent equation of state. This model predicts a relation between the ratio r = ρV /ρDM of the energy densities of the two dark components and expansion rate n of the universe [with a(t) ∝ t n] in the form n = (2/3)(1 +r). For r ≈ 2, we get n ≈ 2 which is consistent with observations.en_US
dc.identifier.urihttp://hdl.handle.net/11007/1210
dc.language.isoenen_US
dc.relation.ispartofseriesIUCAA Preprints;17/02
dc.subjectClustered dark matteren_US
dc.subjectSmooth dark energyen_US
dc.titleCan the clustered dark matter and the smooth dark energy arise from the same scalar field?en_US
dc.typeArticleen_US

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