1997/07/31 by Steven Abel, Ben Allanach, B. C. Allanach · 2 citations
Mathematics · Physics and Astronomy · #Black Holes and Theoretical Physics #Electroweak interaction #Fixed point #Grand Unified Theory #Group (periodic table) #Infrared fixed point #Mathematical analysis #Mathematical physics #Mathematics #Minimal Supersymmetric Standard Model #Particle physics #Particle physics theoretical and experimental studies #Physics #Quantum Chromodynamics and Particle Interactions #Quantum mechanics #Quark #Renormalization group #Scale (ratio) #Supersymmetry #Top quark #Yukawa potential #hep-ph
paper · pdf · doi:10.1016/s0370-2693(97)01274-4
published as Phys.Lett. B415 (1997) 371-382 · 19 Pages plain latex; includes 6 eps figures. References and comments added. Version to appear in Phys.Lett.B
arxiv created 1997/09/19 · openalex publication_date 1997/12/01 · arxiv updated 2009/11/30 · openalex created_date 2016/06/24 · openalex updated_date 2026/08/05
The infra-red fixed points are determined for all the parameters of the MSSM. They dominate the renormalisation group running when the top-Yukawa is in the quasi-fixed point regime (i.e. large at the GUT scale). We examine this behaviour analytically, by solving the full set of one-loop renormalisation group equations in the approximation that the electroweak contributions are negligible, and also numerically. We find the quasi-fixed points for the top-quark trilinear couplings; A_Uα3 = A_U3α=-0.59 mg independently of the input parameters at the unification scale. All the remaining parameters are significantly focused towards their true fixed points at the weak scale. We examine how this increases the predictivity of the MSSM in this regime.