Search results for " Heavy Quark Physics"

showing 2 items of 2 documents

Maximal Flavour Violation: a Cabibbo mechanism for leptoquarks

2018

We propose a mechanism that allows for sizeable flavour violation in quark-lepton currents, while suppressing flavour changing neutral currents in quark-quark and lepton-lepton sectors. The mechanism is applied to the recently proposed 4321 renormalizable model, which can accommodate the current experimental anomalies in $B$-meson decays, both in charged and neutral currents, while remaining consistent with all other indirect flavour and electroweak precision measurements and direct searches at high-$p_T$. To support this claim, we present an exhaustive phenomenological survey of this fully calculable UV complete model and highlight the rich complementarity between indirect and direct searc…

Particle physicsNuclear and High Energy Physics530 PhysicsHigh Energy Physics::LatticeFlavourFOS: Physical sciences10192 Physics Institute01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHeavy Quark Physicslcsh:Nuclear and particle physics. Atomic energy. Radioactivity3106 Nuclear and High Energy Physics010306 general physicsParticle Physics - PhenomenologyPhysicshep-ex010308 nuclear & particles physicsComputer Science::Information RetrievalElectroweak interactionHigh Energy Physics::Phenomenologyhep-phComplementarity (physics)High Energy Physics - PhenomenologyGauge SymmetryBeyond Standard Modellcsh:QC770-798High Energy Physics::ExperimentParticle Physics - ExperimentBeyond Standard Model; Gauge Symmetry; Heavy Quark Physics
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Leptoquark toolbox for precision collider studies

2018

We implement scalar and vector leptoquark (LQ) models in the universal FeynRules output (UFO) format assuming the Standard Model fermion content and conservation of baryon and lepton numbers. Scalar LQ implementations include next-to-leading order (NLO) QCD corrections. We report the NLO QCD inclusive cross sections in proton-proton collisions at 13 TeV, 14 TeV, and 27 TeV for all on-shell LQ production processes. These comprise (i) LQ pair production ($p p \to \Phi \Phi$) and (ii) single LQ + lepton production ($p p \to \Phi \ell$) for all initial quark flavours ($u$, $d$, $s$, $c$, and $b$). Vector LQ implementation includes adjustable non-minimal QCD coupling. We discuss several aspects …

QuarkNuclear and High Energy PhysicsParticle physicsPhysics beyond the Standard ModelHigh Energy Physics::LatticeScalar (mathematics)FOS: Physical sciences01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Beyond Standard Model Heavy Quark Physics0103 physical sciencesHeavy Quark Physicslcsh:Nuclear and particle physics. Atomic energy. RadioactivityLeptoquarkNuclear Experiment010306 general physicsQuantum chromodynamicsPhysicsLarge Hadron Collider010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyHigh Energy Physics - PhenomenologyPair productionBeyond Standard Modellcsh:QC770-798High Energy Physics::Experiment
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