0000000000904344

AUTHOR

Myeonghun Park

showing 2 related works from this author

Adding pseudo-observables to the four-lepton experimentalist’s toolbox

2018

The "golden" channel, in which the newly-discovered Higgs boson decays to four leptons by means of intermediate vector bosons, is important for determining the properties of the Higgs boson and for searching for subtle new physics effects. Different approaches exist for parametrizing the relevant Higgs couplings in this channel; here we relate the use of pseudo-observables to methods based on specifying the most general amplitude or Lagrangian terms for the $HVV$ interactions. We also provide projections for sensitivity in this channel in several novel scenarios, illustrating the use of pseudo-observables, and analyze the role of kinematic distributions and (ratios of) rates in such $H\to4\…

Nuclear and High Energy PhysicsParticle physicsHiggs PhysicsPhysics beyond the Standard ModelFOS: Physical sciencesKinematicsQC770-79801 natural sciencesHigh Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. Radioactivity0103 physical scienceslcsh:Nuclear and particle physics. Atomic energy. RadioactivitySensitivity (control systems)010306 general physicsHiggs Physics ; Beyond Standard ModelParticle Physics - PhenomenologyPhysics010308 nuclear & particles physicsComputer Science::Information RetrievalHigh Energy Physics::PhenomenologyObservablehep-ph3. Good healthHigh Energy Physics - PhenomenologyAmplitudeBeyond Standard ModelHiggs bosonlcsh:QC770-798LeptonCommunication channelJournal of High Energy Physics
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Beyond the dark matter effective field theory and a simplified model approach at colliders

2016

Direct detection of and LHC search for the singlet fermion dark matter (SFDM) model with Higgs portal interaction are considered in a renormalizable model where the full Standard Model (SM) gauge symmetry is imposed by introducing a singlet scalar messenger. In this model, direct detection is described by an effective operator m_q \bar{q} q \bar{\chi} \chi as usual, but the full amplitude for monojet + \not E_T involves two intermediate scalar propagators, which cannot be seen within the effective field theory (EFT) or in the simplified model without the full SM gauge symmetry. We derive the collider bounds from the ATLAS monojet + \not E_T as well as the CMS t\bar{t} + \not E_T data, findi…

PhysicsNuclear and High Energy PhysicsParticle physicsUnitarity010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::LatticeScalar (mathematics)High Energy Physics::PhenomenologyPropagatorFOS: Physical sciences01 natural scienceslcsh:QC1-999High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesEffective field theoryHiggs bosonHigh Energy Physics::ExperimentGauge theory010306 general physicslcsh:PhysicsGauge symmetryPhysics Letters B
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