31,928 research outputs found

    Big Bang nucleosynthesis with a stiff fluid

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    Models that lead to a cosmological stiff fluid component, with a density ρS\rho_S that scales as a6a^{-6}, where aa is the scale factor, have been proposed recently in a variety of contexts. We calculate numerically the effect of such a stiff fluid on the primordial element abundances. Because the stiff fluid energy density decreases with the scale factor more rapidly than radiation, it produces a relatively larger change in the primordial helium-4 abundance than in the other element abundances, relative to the changes produced by an additional radiation component. We show that the helium-4 abundance varies linearly with the density of the stiff fluid at a fixed fiducial temperature. Taking ρS10\rho_{S10} and ρR10\rho_{R10} to be the stiff fluid energy density and the standard density in relativistic particles, respectively, at T=10T = 10 MeV, we find that the change in the primordial helium abundance is well-fit by ΔYp=0.00024(ρS10/ρR10)\Delta Y_p = 0.00024(\rho_{S10}/\rho_{R10}). The changes in the helium-4 abundance produced by additional radiation or by a stiff fluid are identical when these two components have equal density at a "pivot temperature", TT_*, where we find T=0.55T_* = 0.55 MeV. Current estimates of the primordial 4^4He abundance give the constraint on a stiff fluid energy density of ρS10/ρR10<30\rho_{S10}/\rho_{R10} < 30.Comment: 6 pages, 2 figures. Clarification added: element abundances derived using a full numerical calculation. Version accepted at PR

    Decaying dark matter mimicking time-varying dark energy

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    A Λ\LambdaCDM model with dark matter that decays into inert relativistic energy on a timescale longer than the Hubble time will produce an expansion history that can be misinterpreted as stable dark matter with time-varying dark energy. We calculate the corresponding spurious equation of state parameter, w~ϕ\widetilde w_\phi, as a function of redshift, and show that the evolution of w~ϕ\widetilde w_\phi depends strongly on the assumed value of the dark matter density, erroneously taken to scale as a3a^{-3}. Depending on the latter, one can obtain models that mimic quintessence (w~ϕ>1\widetilde w_\phi > -1), phantom models (w~ϕ<1\widetilde w_\phi < -1) or models in which the equation of state parameter crosses the phantom divide, evolving from w~ϕ>1\widetilde w_\phi > -1 at high redshift to w~ϕ<1\widetilde w_\phi < -1 at low redshift. All of these models generically converge toward w~ϕ1\widetilde w_\phi \approx -1 at the present. The degeneracy between the Λ\LambdaCDM model with decaying dark matter and the corresponding spurious quintessence model is broken by the growth of density perturbations.Comment: 6 pages, 2 figures. Added discussion of linear perturbation growth - version accepted at PR
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