Constraints on the minimal supergravity model and prospects for SUSY particle production at future linear e+e− colliders
By Abdelhak Djouadi, J. Kneur, Manuel Drees. 2001
187 citations recorded by the source corpus.
We perform a complete analysis of the supersymmetric particle spectrum in the Minimal Supergravity (mSUGRA) model where the soft SUSY breaking scalar masses, gaugino masses and trilinear couplings are unified at the GUT scale, so that the electroweak symmetry is broken radiatively. We show that the present constraints on the Higgs boson and superparticle masses from collider searches and precision measurements still allow for large regions of the mSUGRA parameter space where charginos, neutralinos, sleptons and top squarks as well as the heavier Higgs particles, are light enough to be produced at the next generation of e+e− linear colliders with center of mass energy around √s ~ 800 GeV, with sizeable cross sections. An important part of this parameter space remains even when we require that the density of the lightest neutralinos left over from the Big Bang, which we calculate using standard assumptions, falls in the range favored by current determinations of the Dark Matter density in the Universe. Already at a c.m. energy of 500 GeV, SUSY particles can be accessible in some parameter range, and if the energy is increased to √s 1.2 TeV, the e+e− collider will have a reach for high precision studies of SUSY particles in a range that is comparable to the discovery range of the LHC.
Subfields: Astronomy and Astrophysics, Nuclear and High Energy Physics
View Paper: https://www.semanticscholar.org/paper/6cbb0987d3523ec4622a8f8923d869d0f72eef9c
How researchers see this paper
The researchers whose trusted networks rank it highest, strongest advocate first. Every researcher gets a different order.
In Astronomy and Astrophysics
In Nuclear and High Energy Physics
Citations in the corpus
- Fully covering the MSSM Higgs sector at the LHC (2015, background): “iv) Finally, there is the Higgs-pole region [128–133] in which an efficient LSP annihilation into SM particles is provided by the exchange of an almost on-shell A boson in the s-channel; one thus needs MA ≈ 2mχ01 (the possibility of h-boson exchange [134, 135] leading to mχ01 ≈ 60 GeV is by now unli”