Combined analyses of recent cosmological data are showing interesting hints for the presence of an extra relativistic component, coined dark radiation. Here, we perform a new search for dark radiation, parametrizing it with an effective number of relativistic degrees of freedom parameter, N-eff. We show that the cosmological data we considered are clearly suggesting the presence of an extra relativistic component with N-eff = 4.08(-0.68)(+0.71) at 95% C.L.. Performing an analysis on dark radiation sound speed c(eff) and viscosity c(vis) parameters, we found c(eff)(2) = 0.312 +/- 0.026 and c(vis)(2) = 0.29(-0.16)(+0.21) at 95% C.L., consistent with the expectations of a relativistic free streaming component (c(eff)(2) = c(vis)(2) = 1/3). Assuming the presence of 3 relativistic neutrinos, we constrain the extra relativistic component with N-v(S) = 1.10-0.72+0.79 and c(eff)(2) = 0.24(-0.13)(+0.08) at 95% C. L. while c(vis)(2) results as unconstrained. Assuming a massive neutrino component, we obtain further indications for dark radiation with N-v(S) = 1.12(-0.74)(+0.86) at 95% C.L..
Case for dark radiation / Maria, Archidiacono; Erminia, Calabrese; Melchiorri, Alessandro. - In: PHYSICAL REVIEW D, PARTICLES, FIELDS, GRAVITATION, AND COSMOLOGY. - ISSN 1550-7998. - 84:12(2011). [10.1103/physrevd.84.123008]
Case for dark radiation
MELCHIORRI, Alessandro
2011
Abstract
Combined analyses of recent cosmological data are showing interesting hints for the presence of an extra relativistic component, coined dark radiation. Here, we perform a new search for dark radiation, parametrizing it with an effective number of relativistic degrees of freedom parameter, N-eff. We show that the cosmological data we considered are clearly suggesting the presence of an extra relativistic component with N-eff = 4.08(-0.68)(+0.71) at 95% C.L.. Performing an analysis on dark radiation sound speed c(eff) and viscosity c(vis) parameters, we found c(eff)(2) = 0.312 +/- 0.026 and c(vis)(2) = 0.29(-0.16)(+0.21) at 95% C.L., consistent with the expectations of a relativistic free streaming component (c(eff)(2) = c(vis)(2) = 1/3). Assuming the presence of 3 relativistic neutrinos, we constrain the extra relativistic component with N-v(S) = 1.10-0.72+0.79 and c(eff)(2) = 0.24(-0.13)(+0.08) at 95% C. L. while c(vis)(2) results as unconstrained. Assuming a massive neutrino component, we obtain further indications for dark radiation with N-v(S) = 1.12(-0.74)(+0.86) at 95% C.L..I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.