1999/07/31 by M. E. Gómez, M. E. Gomez, G. Lazarides +1 · 2 citations
Physics and Astronomy · #Cold dark matter #Cosmology and Gravitation Theories #Dark Matter and Cosmic Phenomena #Dark matter #Electroweak interaction #Grand Unified Theory #Gravitino #Lightest Supersymmetric Particle #Minimal Supersymmetric Standard Model #Particle physics #Particle physics theoretical and experimental studies #Physics #Supergravity #Supersymmetry #Yukawa potential #hep-ph
paper · pdf · doi:10.1103/physrevd.61.123512
published as Phys.Rev.D61:123512,2000 · 27 pages including 5 figures, Revtex, minor corrections
arxiv created 2000/05/08 · openalex publication_date 2000/05/26 · arxiv updated 2009/11/30 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05
The cosmological relic density of the lightest supersymmetric particle of the minimal supersymmetric standard model is calculated under the assumption of gauge and Yukawa coupling unification. We employ radiative electroweak breaking with universal boundary conditions from gravity-mediated supersymmetry breaking. Coannihilation of the lightest supersymmetric particle, which turns out to be an almost pure B-ino, with the next-to-lightest supersymmetric particle (the lightest stau) is crucial for reducing its relic density to an acceptable level. Agreement with the mixed or the pure cold (in the presence of a nonzero cosmological constant) dark matter scenarios for large scale structure formation in the universe requires that the lightest stau mass is about 2\ensuremath-8% larger than the B-ino mass, which can be as low as 222 GeV. The smallest allowed value of the lightest stau mass turns out to be about 232 GeV.