Search results for "Higgsino"

showing 4 items of 24 documents

The Minimal Supersymmetric Model without a mu term

2002

We propose a supersymmetric extension of the standard model which is a realistic alternative to the MSSM, and which has several advantages. No ``mu'' supersymmetric Higgs/Higgsino mass parameter is needed for sufficiently heavy charginos. An approximate U(1) R symmetry naturally guarantees that tan beta is large, explaining the top/bottom quark mass hierarchy. This symmetry also suppresses supersymmetric contributions to anomalous magnetic moments, b to s gamma, and proton decay, and these processes place no lower bounds on superpartner masses, even at large tan beta. The soft supersymmetry breaking mass parameters can easily be obtained from either gauge or Planck scale mediation, without …

PhysicsNuclear and High Energy PhysicsParticle physicsProton decayHigh Energy Physics::PhenomenologySuperpartnerFOS: Physical sciencesFísicaSupersymmetry breakingUpper and lower boundsStandard ModelHigh Energy Physics::TheoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentHiggsinoMu problem
researchProduct

Search for pair production of Higgsinos in final states with at least three b -tagged jets in s=13  TeV pp collisions using the ATLAS detector

2018

A search for pair production of the supersymmetric partners of the Higgs boson (higgsinos H˜) in gauge-mediated scenarios is reported. Each higgsino is assumed to decay to a Higgs boson and a gravitino. Two complementary analyses, targeting high- and low-mass signals, are performed to maximize sensitivity. The two analyses utilize LHC pp collision data at a center-of-mass energy s=13  TeV, the former with an integrated luminosity of 36.1  fb-1 and the latter with 24.3  fb-1, collected with the ATLAS detector in 2015 and 2016. The search is performed in events containing missing transverse momentum and several energetic jets, at least three of which must be identified as b-quark jets. No sig…

PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologySupersymmetry01 natural sciencesPair productionmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesmedicineHiggs bosonHigh Energy Physics::ExperimentGravitinoHiggsino010306 general physicsPhysical Review D
researchProduct

Perturbative unitarity constraints on the NMSSM Higgs Sector

2018

Abstract We place perturbative unitarity constraints on both the dimensionful and dimensionless parameters in the Next-to-Minimal Supersymmetric Standard Model (NMSSM) Higgs Sector. These constraints, plus the requirement that the singlino and/or Higgsino constitutes at least part of the observed dark matter relic abundance, generate upper bounds on the Higgs, neutralino and chargino mass spectrum. Requiring higher-order corrections to be no more than 41% of the tree-level value, we obtain an upper bound of 20 TeV for the heavy Higgses and 12 TeV for the charginos and neutralinos outside defined fine-tuned regions. If the corrections are no more than 20% of the tree-level value, the bounds …

PhysicsParticle physicsUnitarity010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyAstronomy and Astrophysics01 natural sciencesHiggs sectorCharginoSpace and Planetary Science0103 physical sciencesNeutralinoHiggs bosonHigh Energy Physics::ExperimentHiggsino010306 general physicsMinimal Supersymmetric Standard ModelPhysics of the Dark Universe
researchProduct

Supersymmetric electroweak baryogenesis

1999

We calculate the baryon asymmetry generated at the electroweak phase transition in the minimal supersymmetric standard model, using a new method to compute the CP-violating asymmetry in the Higgsino flux reflected into the unbroken phase. The method is based on a Higgs insertion expansion. We find that the CP asymmetry at leading order is proportional to the change in $\tan \beta$ in the bubble wall, which is at most of order $10^{-2}$, while at next-to-leading order this suppression factor disappears. This result may enhance the final baryon asymmetry generated during the electroweak phase transition for small $\Delta \beta (< 10^{-3}$).

PhysicsPhase transitionParticle physicsNuclear and High Energy Physicsmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyElectroweak interactionFOS: Physical sciencesFísicaAsymmetryAtomic and Molecular Physics and OpticsBaryogenesisHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetryHiggs bosonHigh Energy Physics::ExperimentHiggsinoMinimal Supersymmetric Standard Modelmedia_commonNuclear Physics B - Proceedings Supplements
researchProduct