2003/04/30 by Jussi Valiviita, J. Väliviita, Vesa Muhonen · 7 citations
Physics and Astronomy · #Cosmology and Gravitation Theories #Galaxies: Formation, Evolution, Phenomena #Relativity and Gravitational Theory #astro-ph #hep-ph
paper · pdf · doi:10.1103/physrevlett.91.131302
published as Phys.Rev.Lett. 91 (2003) 131302 · 5 pages, 7 figures. V2: Added 2 figures and revised a bit the results section. This is a slightly longer version than the published one in PRL
openalex publication_date 2003/09/24 · arxiv created 2003/10/01 · arxiv updated 2009/11/30 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/30
In general correlated models, in addition to the usual adiabatic component with a spectral index nad1 there is another adiabatic component with a spectral index nad2 generated by entropy perturbation during inflation. We extend the analysis of a correlated mixture of adiabatic and isocurvature cosmic microwave background fluctuations of the Wilkinson Microwave Anisotropy Probe (WMAP) group, who set the two adiabatic spectral indices equal. Allowing nad1 and nad2 to vary independently we find that the WMAP data favor models where the two adiabatic components have opposite spectral tilts. Using the WMAP data only, the 2\ensuremathσ upper bound for the isocurvature fraction fiso of the initial power spectrum at k0=0.05 Mpc^\ensuremath-1 increases somewhat, e.g., from 0.76 of nad2=nad1 models to 0.84 with a prior niso<1.84 for the isocurvature spectral index.