2004/11/16 by Daniel J. H. Chung, Edward W. Kolb, Antonio Riotto +1 · 2 citations
Physics and Astronomy · #Anisotropy #Astrophysics #Cold dark matter #Cosmic microwave background #Cosmology #Cosmology and Gravitation Theories #Dark Matter and Cosmic Phenomena #Dark energy #Dark matter #Galaxies: Formation, Evolution, Phenomena #Gravitino #Hot dark matter #Inflation (cosmology) #Light dark matter #Particle physics #Physics #Quantum mechanics #Scalar field dark matter #Supergravity #Supersymmetry #Theoretical physics #astro-ph #hep-ph #hep-th
paper · pdf · doi:10.1103/physrevd.72.023511
published as Phys.Rev.D72:023511,2005 · 29 pages, 2 figures
arxiv created 2004/11/16 · openalex publication_date 2005/07/14 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
We show that the isocurvature perturbations imply that the gravitationally produced superheavy dark matter must have masses larger than a few times the Hubble expansion rate at the end of inflation. This together with the bound on tensor to scalar contribution to the CMB induces a lower bound on the reheating temperature for superheavy dark matter to be about 107 GeV. Hence, if the superheavy dark-matter scenario is embedded in supergravity models with gravity mediated supersymmetry breaking, the gravitino bound will squeeze this scenario. Furthermore, the CMB constraint strengthens the statement that a gravitationally produced superheavy dark-matter scenario prefers a relatively large tensor mode amplitude if the reheating temperature must be less than 109 GeV.