Search results for "Higgs"

showing 10 items of 1127 documents

Observational properties of feebly coupled dark matter

2016

We show that decoupled hidden sectors can have observational consequences. As a representative model example, we study dark matter production in the Higgs portal model with one real singlet scalar $s$ coupled to the Standard Model Higgs via $\lambda_{\rm hs}\Phi^\dagger\Phi s^2$ and demonstrate how the combination of non-observation of cosmological isocurvature perturbations and astrophysical limits on dark matter self-interactions imply stringent bounds on the magnitude of the scalar self-coupling $\lambda_{\rm s}s^4$. For example, for dark matter mass $m_{\rm s}=10$ MeV and Hubble scale during cosmic inflation $H_*=10^{12}$ GeV, we find $10^{-4}\lesssim \lambda_{\rm s}\lesssim 0.2$.

PhysicsParticle physicsCosmology and Nongalactic Astrophysics (astro-ph.CO)Dark matterHigh Energy Physics::PhenomenologyScalar field dark matterFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysicsdark matterStandard ModelHidden sectorpimeä aineHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonProduction (computer science)Light dark matterDark fluidAstrophysics - Cosmology and Nongalactic Astrophysics
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Updated Z Parameters, and Standard Model Fits from Electroweak Precision Data

1999

Data taking around the Z resonance at LEP I ended in 1995, and determinations of the mass, width, hadronic pole cross section and leptonic couplings of the Z boson are approaching a final status. This is accompanied by an improved understanding of the beam energy during the high-statistics data taking approximately two GeV above and below the Z resonance in 1993 and 1995. Together with other precision measurements presented at this conference impressive tests of the consistency of the Standard Model can be made and an upper limit on the mass of the Higgs boson can be derived.

PhysicsParticle physicsCross section (physics)Consistency (statistics)High Energy Physics::PhenomenologyElectroweak interactionHadronHiggs bosonHigh Energy Physics::ExperimentLimit (mathematics)Resonance (particle physics)Standard Model
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Yukawa coupling corrections to the decay $H^+ \to W^+ A^0$

1998

We compute the fermionic radiative contributions to the decay $H^+ \to W^{+(*)} A^0$ in the framework of models with two Higgs doublets (2HDM), for the case of an on-shell and off-shell W. We show that, in the majority of the cases, current measurements of the $\rho$ parameter suggest $M_{H^{\pm}}\ge M_A$ and such decays could invalidate current charged Higgs searches or aid detection in the region $M_{H^{\pm}}\approx M_W$. We find that the radiative corrections may approach 50% for small values of $\tan\beta$.

PhysicsParticle physicsCurrent (mathematics)Physics and Astronomy (miscellaneous)High Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesApproxCoupling (probability)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Radiative transferHiggs bosonHigh Energy Physics::ExperimentEngineering (miscellaneous)The European Physical Journal C
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X-ray photons from late-decaying majoron dark matter

2008

An attractive way to generate neutrino masses as required to account for current neutrino oscillation data involves the spontaneous breaking of lepton number. The resulting majoron may pick up a mass due to gravity. If its mass lies in the kilovolt scale, the majoron can play the role of late-decaying Dark Matter (LDDM), decaying mainly to neutrinos. In general the majoron has also a sub-dominant decay to two photons leading to a mono-energetic emission line which can be used as a test of the LDDM scenario. We compare expected photon emission rates with observations in order to obtain model independent restrictions on the relevant parameters. We also illustrate the resulting sensitivities w…

PhysicsParticle physicsDark matterAstrophysics (astro-ph)High Energy Physics::PhenomenologyCosmic background radiationFOS: Physical sciencesFísicaAstronomy and AstrophysicsAstrophysicsLepton numberHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryHiggs bosonHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationMajoron
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Radiative Seesaw Dark Matter

2021

The singlet majoron model of seesaw neutrino mass is appended by one dark Majorana fermion singlet $\chi$ with $L=2$ and one dark complex scalar singlet $\zeta$ with $L=1$. This simple setup allows $\chi$ to obtain a small radiative mass anchored by the same heavy right-handed neutrinos, whereas the one-loop decay of the standard-model Higgs boson to $\chi \chi + \bar{\chi} \bar{\chi}$ provides the freeze-in mechanism for $\chi$ to be the light dark matter of the Universe.

PhysicsParticle physicsDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryHiggs bosonHigh Energy Physics::ExperimentNeutrinoLight dark matterMajorana fermionMajoron
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Dark matter stability from Dirac neutrinos in scotogenic 3-3-1-1 theory

2020

We propose the simplest TeV-scale scotogenic extension of the original 3-3-1 theory, where dark matter stability is linked to the Dirac nature of neutrinos, which results from an unbroken $B-L$ gauge symmetry. The new gauge bosons get masses through the interplay of spontaneous symmetry breaking \`a la Higgs and the Stueckelberg mechanism.

PhysicsParticle physicsGauge boson010308 nuclear & particles physicsDirac (video compression format)Spontaneous symmetry breakingHigh Energy Physics::LatticeDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciences01 natural sciencesComputer Science::Digital LibrariesHigh Energy Physics - PhenomenologyHigh Energy Physics::TheoryExtension (metaphysics)High Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentNeutrino010306 general physicsGauge symmetry
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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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Testing triplet fermions at the electron-positron and electron-proton colliders using fat jet signatures

2020

The addition of $SU(2)_L$ triplet fermions of zero hypercharge with the Standard Model (SM) helps to explain the origin of the neutrino mass by the so-called seesaw mechanism. Such a scenario is commonly know as the type-III seesaw model. After the electroweak symmetry breaking the mixings between the light and heavy mass eigenstates of the neutral leptons are developed which play important roles in the study of the charged and neutral multiplets of the triplet fermions at the colliders. In this article we study such interactions to produce these multiplets of the triplet fermion at the electron-positron and electron-proton colliders at different center of mass energies. We focus on the hea…

PhysicsParticle physicsGauge bosonHypercharge010308 nuclear & particles physicsElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFermion01 natural sciencesHigh Energy Physics - ExperimentStandard ModelHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Seesaw mechanism0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsLepton
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FlexibleSUSY -- A spectrum generator generator for supersymmetric models

2014

We introduce FlexibleSUSY, a Mathematica and C++ package, which generates a fast, precise C++ spectrum generator for any SUSY model specified by the user. The generated code is designed with both speed and modularity in mind, making it easy to adapt and extend with new features. The model is specified by supplying the superpotential, gauge structure and particle content in a SARAH model file; specific boundary conditions e.g. at the GUT, weak or intermediate scales are defined in a separate FlexibleSUSY model file. From these model files, FlexibleSUSY generates C++ code for self-energies, tadpole corrections, renormalization group equations (RGEs) and electroweak symmetry breaking (EWSB) co…

PhysicsParticle physicsGenerator (computer programming)SuperpotentialElectroweak interactionHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFOS: Physical sciencesSupersymmetryTopologyHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Hardware and ArchitectureHiggs bosonSymmetry breakingBoundary value problemddc:004Minimal Supersymmetric Standard Model
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Searching for new physics in bottomonium decays

2005

Heavy quarkonium decays can be used to search for New Physics beyond the Standard Model. In particular, a light Higgs boson could induce a slight (but observable) lepton universality breaking in Upsilon decays. In fact, current experimental data from CLEO presented in this Conference seem to point out to this direction within experimental accuracy. Moreover, LEP constraints on a light Higgs mass can be evaded by different models (like MSSM with a CPV Higgs sector) as shown in this Conference. We also consider spectroscopic consequences stemming from a possible mixing between Higgs and bottomonium states leading to discrepancies with the SM expectations (e.g. hyperfine splittings).

PhysicsParticle physicsHigh Energy Physics::LatticePhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyUniversality (philosophy)FOS: Physical sciencesObservableQuarkoniumHiggs sectorHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonHigh Energy Physics::ExperimentMixing (physics)LeptonProceedings of International Europhysics Conference on High Energy Physics — PoS(HEP2005)
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