Z$ decay into a bottom quark, a light sbottom and a light gluino
arXiv:hep-ph/0207219 · doi:10.1103/PhysRevD.67.015005
Abstract
The discrepancy between the measured and theoretical production cross section of quarks at the Tevatron can probably be explained by the recently proposed scenario of light gluinos of mass 12-16 GeV and light sbottoms of mass GeV. In this scenario, we study a related process at the pole, followed by . The hadronic branching ratio for this channel is , which is of order of the size of the uncertainty in . We find that a typical event consists of an energetic prompt bottom-jet back-to-back with a ``fat'' bottom-jet, which consists of a bottom quark and two bottom squarks. Such events with a branching ratio may affect the measurement of ; even more interesting if the ``fat'' bottom jet can be identified.
14 pages, references are added
References in corpus (8)
- Is There a Significant Excess in Bottom Hadroproduction at the Tevatron?
- The Sources of b-Quarks at the Tevatron and their Correlations
- Very light sbottom and gluino scenario confronting electroweak precision tests
- Light bottom squark and gluino confront electroweak precision measurements
- Higgs Boson Decay into Hadronic Jets
- Light Gluino, Light Bottom Squark Scenario, and LEP Predictions
- Hadronic decays of into light bottom squarks
- Increased Yield of ttbb at Hadron Colliders in Low-Energy Supersymmetry
Cited by in corpus (9)
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- Z decays into light gluinos: a calculation based on unitarity
- Impact of CP phases on a light sbottom and gluino sector
- Phenomenological study of the atypical heavy flavor production observed at the Fermilab Tevatron
- Can there be a heavy sbottom hidden in three-jet data at LEP?
- R Parity Violating Decays of the Gluino