2002/02/28 by J. V. Cunha, J. S. Alcaniz, J. A. S. Lima · 23 citations
Physics and Astronomy · #Angular diameter #Astrophysics #Black Holes and Theoretical Physics #Cosmology and Gravitation Theories #Galaxies: Formation, Evolution, Phenomena #Galaxy #Globular cluster #Lambda #Mathematical physics #Omega #Physics #Quantum mechanics #Redshift #Stars #astro-ph
paper · pdf · doi:10.1103/physrevd.66.023520
published in Physical review. D. Particles, fields, gravitation, and cosmology/Physical review. D. Particles and fields 66(2) (American Physical Society) · 6 pages, 3 figures, revised version to appear in Phys. Rev. D
arxiv created 2002/07/02 · openalex publication_date 2002/07/29 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
Observational constraints to a large class of decaying vacuum cosmologies are derived using the angular size data of compact radio sources and the latest age estimates of globular clusters. For this class of deflationary \ensuremathΛ(t) models, the present value of the vacuum energy density is quantified by a positive \ensuremathβ parameter smaller than unity. In the case of milliarcsecond compact radio-sources, we find that the allowed intervals for \ensuremathβ and the matter density parameter \ensuremathΩm are heavily dependent on the value of the mean projected linear size l. For l\ensuremath≃20h^\ensuremath-1\ensuremath-30h^\ensuremath-1 pc, the best fit occurs for \ensuremathβ\ensuremath∼0.58, \ensuremathΩm\ensuremath∼0.58, and \ensuremathβ\ensuremath∼0.76, \ensuremathΩm\ensuremath∼0.28, respectively. This analysis shows that if one minimizes \ensuremathχ2 for the free parameters l, \ensuremathΩm and \ensuremathβ, the best fit for these angular size data corresponds to a decaying \ensuremathΛ(t) with \ensuremathΩm=0.54, \ensuremathβ=0.6, and l=22.64h^\ensuremath-1 pc. Constraints from age estimates of globular clusters and old high redshift galaxies are not so restrictive, thereby suggesting that there is no age crisis for this kind of \ensuremathΛ(t) cosmologies.