Probing lepton flavour violation in slepton NLSP scenarios
arXiv:hep-ph/0412229 · doi:10.1088/1126-6708/2005/02/028
Abstract
In supersymmetric models where the gravitino is the lightest superparticle, the next-to-lightest superparticle (NLSP) is long-lived, and hence could be collected and studied in detail. We study the prospects of direct detection of lepton flavour violation in charged slepton NLSP decays. Mixing angles in the slepton sector as small as ~ 3\times 10^{-2} (9\times 10^{-3}) could be probed at the 90% confidence level if 3\times 10^3 (3\times 10^4) sleptons could be collected.
20 pages, 8 figures. v2:Comments and references are added
References in corpus (6)
- Big Bang Nucleosynthesis (in "The Review of Particle Properties" 2004)
- Gravitino Dark Matter in the CMSSM and Implications for Leptogenesis and the LHC
- A study of late decaying charged particles at future colliders
- Slepton Trapping at the Large Hadron and International Linear Colliders
- Prospects for Sparticle Discovery in Variants of the MSSM
- Gravitino and Goldstino at Colliders
Cited by in corpus (17)
- SPheno 3.1: extensions including flavour, CP-phases and models beyond the MSSM
- Gravitino Dark Matter in R-Parity Breaking Vacua
- Collider aspects of flavour physics at high Q
- Long life stau in the minimal supersymmetric standard model
- The Standard Model and Supersymmetric Flavor Puzzles at the Large Hadron Collider
- Test of lepton flavour violation at LHC
- μto e in R-symmetric Supersymmetry
- Measuring lifetimes of long-lived charged massive particles stopped in LHC detectors
- The Gravitino in Gaugino Mediation
- LHC sensitivity to lepton flavour violating Z boson decays
- Flavorful Supersymmetry
- Long-Lived Staus at Neutrino Telescopes
- Long-lived Staus from Cosmic Rays
- Beyond the standard seesaw: neutrino masses from Kahler operators and broken supersymmetry
- A Clean Slepton Mixing Signal at the LHC
- Lepton flavour violation in future linear colliders in the long-lived stau NLSP scenario
- Gaugino Mediation Combined with the Bulk Matter Randall-Sundrum Model