Search results for "Dark matter"

showing 10 items of 627 documents

Perturbative unitarity constraints on gauge portals

2017

Abstract Dark matter that was once in thermal equilibrium with the Standard Model is generally prohibited from obtaining all of its mass from the electroweak phase transition. This implies a new scale of physics and mediator particles to facilitate dark matter annihilation. In this work, we focus on dark matter that annihilates through a generic gauge boson portal. We show how partial wave unitarity places upper bounds on the dark gauge boson, dark Higgs and dark matter masses. Outside of well-defined fine-tuned regions, we find an upper bound of 9 TeV for the dark matter mass when the dark Higgs and dark gauge bosons both facilitate the dark matter annihilations. In this scenario, the uppe…

PhysicsParticle physicsGauge boson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyElectroweak interactionDark matterAstronomy and AstrophysicsElementary particleAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesStandard ModelSpace and Planetary Science0103 physical sciencesHiggs bosonGrand Unified Theory010306 general physicsBosonPhysics of the Dark Universe
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Lepton jets from radiating dark matter

2015

Journal of High Energy Physics 2015.7 (2015): 045 reproduced by permission of Scuola Internazionale Superiore di Studi Avanzati (SISSA)

PhysicsParticle physicsGauge bosonNuclear and High Energy PhysicsToy modelPhotonElectromagnetic Processes and PropertiesDark matterHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesFermionAstrophysics::Cosmology and Extragalactic AstrophysicsDark photonStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Parton ModelBeyond Standard ModelHigh Energy Physics::ExperimentLeptonJournal of High Energy Physics
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New Methods of Axion Dark Matter Detection

2017

In this chapter, I consider new linear effects of axion (pseudoscalar) dark matter in atoms, molecules, nuclei and neutrons.

PhysicsParticle physicsHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryDark matterScalar field dark matterPseudoscalarHigh Energy Physics::TheoryMixed dark matterWarm dark matterNeutronNuclear ExperimentAxion
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Search for Dark Matter in Events with a Hadronically DecayingWorZBoson and Missing Transverse Momentum inppCollisions ats=8  TeVwith the ATLAS Detect…

2014

A search is presented for dark matter pair production in association with a W or Z boson in pp collisions representing 20.3 fb(-1) of integrated luminosity at root s = 8 TeV using data recorded with the ATLAS detector at the Large Hadron Collider. Events with a hadronic jet with the jet mass consistent with a W or Z boson, and with large missing transverse momentum are analyzed. The data are consistent with the standard model expectations. Limits are set on the mass scale in effective field theories that describe the interaction of dark matter and standard model particles, and on the cross section of Higgs production and decay to invisible particles. In addition, cross section limits on the…

PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsAtlas (topology)High Energy Physics::PhenomenologyHadronDark matterGeneral Physics and Astronomy01 natural sciencesNuclear physicsPair production0103 physical sciencesEffective field theoryHiggs bosonHigh Energy Physics::Experiment010306 general physicsBosonPhysical Review Letters
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Exposing the dark sector with future Z factories

2017

We investigate the prospects of searching dark sector models via exotic Z-boson decay at future e⁺e⁻ colliders with Giga Z and Tera Z options. Four general categories of dark sector models, Higgs portal dark matter, vector-portal dark matter, inelastic dark matter, and axionlike particles, are considered. Focusing on channels motivated by the dark sector models, we carry out a model-independent study of the sensitivities of Z factories in probing exotic decays. The limits on branching ratios of the exotic Z decay are typically O(10⁻⁶–10⁻[superscript 8.5]) for the Giga Z and O(10⁻[superscript 7.5]–10⁻¹¹) for the Tera Z, and they are compared with the projection for the high luminosity LHC. W…

PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsPhysics beyond the Standard ModelDark matterFOS: Physical scienceshep-phAstrophysics::Cosmology and Extragalactic Astrophysics01 natural scienceslaw.inventionHidden sectorHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)law0103 physical sciencesEffective field theoryHiggs bosonHigh Energy Physics::Experiment010306 general physicsColliderParticle Physics - PhenomenologyPhysical Review D
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Search for Low-Mass Dijet Resonances Using Trigger-Level Jets with the ATLAS Detector in pp Collisions at s=13  TeV

2018

Searches for dijet resonances with sub-TeV masses using the ATLAS detector at the Large Hadron Collider can be statistically limited by the bandwidth available to inclusive single-jet triggers, who ...

PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAtlas detectorAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyDark matterGeneral Physics and AstronomyResonanceElementary particle01 natural sciencesDigital storageWeakly interacting massive particles0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::Experiment010306 general physicsLow MassPhysical Review Letters
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Search for Invisible Decays of a Dark Photon Produced in e+e− Collisions at BaBar

2017

We search for single-photon events in 53  fb^{-1} of e^{+}e^{-} collision data collected with the BABAR detector at the PEP-II B-Factory. We look for events with a single high-energy photon and a large missing momentum and energy, consistent with production of a spin-1 particle A^{'} through the process e^{+}e^{-}→γA^{'}; A^{'}→invisible. Such particles, referred to as "dark photons," are motivated by theories applying a U(1) gauge symmetry to dark matter. We find no evidence for such processes and set 90% confidence level upper limits on the coupling strength of A^{'} to e^{+}e^{-} in the mass range m_{A^{'}}≤8  GeV. In particular, our limits exclude the values of the A^{'} coupling sugges…

PhysicsParticle physicsMuon010308 nuclear & particles physicsElectron–positron annihilationDark matterGeneral Physics and AstronomyCoupling (probability)01 natural sciencesDark photonB-factoryNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)010306 general physicsBosonPhysical Review Letters
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Search for a Dark Photon ine+e−Collisions atBaBar

2014

Dark sectors charged under a new Abelian interaction have recently received much attention in the context of dark matter models. These models introduce a light new mediator, the so-called dark photon (A^{'}), connecting the dark sector to the standard model. We present a search for a dark photon in the reaction e^{+}e^{-}→γA^{'}, A^{'}→e^{+}e^{-}, μ^{+}μ^{-} using 514  fb^{-1} of data collected with the BABAR detector. We observe no statistically significant deviations from the standard model predictions, and we set 90% confidence level upper limits on the mixing strength between the photon and dark photon at the level of 10^{-4}-10^{-3} for dark photon masses in the range 0.02-10.2  GeV. W…

PhysicsParticle physicsMuonPhotonAnomalous magnetic dipole momentElectron–positron annihilationDark matterGeneral Physics and AstronomyContext (language use)Astrophysics::Cosmology and Extragalactic Astrophysics7. Clean energyDark photonStandard ModelNuclear physicsPhysical Review Letters
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The coannihilation codex

2015

We present a general classification of simplified models that lead to dark matter (DM) coannihilation processes of the form DM + X $\rightarrow$ SM$_1$ + SM$_2$, where X is a coannihilation partner for the DM particle and SM$_1$, SM$_2$ are Standard Model fields. Our classification also encompasses regular DM pair annihilation scenarios if DM and X are identical. Each coannhilation scenario motivates the introduction of a mediating particle M that can either belong to the Standard Model or be a new field, whereby the resulting interactions between the dark sector and the Standard Model are realized as tree-level and dimension-four couplings. We construct a basis of coannihilation models, cl…

PhysicsParticle physicsNuclear and High Energy PhysicsAnnihilationLarge Hadron Collider010308 nuclear & particles physicsPhysicsElectroweak interactionDark matterFOS: Physical sciencesFermionQuantum number01 natural sciencesHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesddc:530Hadronic CollidersSymmetry breaking010306 general physicsPhenomenological ModelsJournal of High Energy Physics
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Prediction for the lightest Higgs boson mass in the CMSSM using indirect experimental constraints

2007

Measurements at low energies provide interesting indirect information about masses of particles that are (so far) too heavy to be produced directly. Motivated by recent progress in consistently and rigorously calculating electroweak precision observables and flavour related observables, we derive the preferred value for m_h in the Constrained Minimal Supersymmetric Standard Model (CMSSM), obtained from a fit taking into account electroweak precision data, flavour physics observables and the abundance of Cold Dark Matter. No restriction is imposed on m_h itself: the experimental bound from direct Higgs boson search at LEP is not included in the fit. A multi-parameter chi^2 is minimized with …

PhysicsParticle physicsNuclear and High Energy PhysicsCold dark matterHigh Energy Physics::LatticeDark matterElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesObservableStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentParticle Physics - ExperimentMinimal Supersymmetric Standard ModelFree parameterParticle Physics - Phenomenology
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