Search results for "SEEs"

showing 10 items of 143 documents

Leptogenesis with a dynamical seesaw scale

2014

In the simplest type-I seesaw leptogenesis scenario right-handed neutrino annihilation processes are absent. However, in the presence of new interactions these processes are possible and can affect the resulting $B-L$ asymmetry in an important way. A prominent example is provided by models with spontaneous lepton number violation, where the existence of new dynamical degrees of freedom can play a crucial role. In this context, we provide a model-independent discussion of the effects of right-handed neutrino annihilations. We show that in the weak washout regime, as long as the scattering processes remain slow compared with the Hubble expansion rate throughout the relevant temperature range,…

PhysicsParticle physicsAnnihilation010308 nuclear & particles physicsmedia_common.quotation_subjectDegrees of freedom (statistics)FOS: Physical sciencesFísicaAstronomy and AstrophysicsContext (language use)01 natural sciencesLepton numberAsymmetryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryLeptogenesis0103 physical sciencesNeutrino010306 general physicsmedia_common
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R parity violation assisted thermal leptogenesis in the seesaw mechanism.

2005

Successful leptogenesis within the simplest type I supersymmetric seesaw mechanism requires the lightest of the three right-handed neutrino supermultiplets to be heavier than $\sim10^9$ GeV. Thermal production of such (s)neutrinos requires very high reheating temperatures which result in an overproduction of gravitinos with catastrophic consequences for the evolution of the universe. In this letter, we let R-parity be violated through a $\lambda_i \hat{N}_i \hat{H}_u \hat{H}_d$ term in the superpotential, where $\hat{N}_i$ are right-handed neutrino supermultiplets. We show that in the presence of this term, the produced lepton-antilepton asymmetry can be enhanced. As a result, even for $\ha…

PhysicsParticle physicsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologySuperpotentialFísicaFOS: Physical sciencesGeneral Physics and AstronomyBaryonHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Baryon asymmetrySeesaw mechanismR-parityLeptogenesisHigh Energy Physics::ExperimentGravitinoNeutrinoPhysical review letters
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Dark Matter and the Seesaw Scale

2018

We discuss the possibility to find an upper bound on the seesaw scale using the cosmological bound on the cold dark matter relic density. We investigate a simple relation between the origin of neutrino masses and the properties of a dark matter candidate in a simple theory where the new symmetry breaking scale defines the seesaw scale. Imposing the cosmological bounds, we find an upper bound of order multi-TeV on the lepton number violation scale. We investigate the predictions for direct and indirect detection dark matter experiments, and the possible signatures at the Large Hadron Collider.

PhysicsParticle physicsCold dark matter010308 nuclear & particles physicsDark matterHigh Energy Physics::PhenomenologyFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics01 natural sciencesLepton numberUpper and lower boundsPartícules (Física nuclear)High Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryWeakly interacting massive particles0103 physical sciencesGran col·lisionador d'hadrons (França i Suïssa)High Energy Physics::ExperimentSymmetry breakingNeutrino010306 general physics
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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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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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Neutrino mass in supersymmetry

2009

10 páginas, 8 figuras.-- El PDF es la versión pre-print (arXiv:0911.3103v1).-- Trabajo presentado al SUSY09: 7th International Conference on Supersymmetry and the Unification of Fundamental Interactions.

PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyFOS: Physical sciencesContext (language use)Supersymmetry01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryR-parity0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationMixing (physics)
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Probing the Type I Seesaw mechanism with displaced vertices at the LHC

2015

The observation of Higgs decays into heavy neutrinos would be strong evidence for new physics associated to neutrino masses. In this work we propose a search for such decays within the Type I seesaw model in the few-GeV mass range via displaced vertices. Using 300 fb$^{-1}$ of integrated luminosity, at 13 TeV, we explore the region of parameter space where such decays are measurable. We show that, after imposing pseudorapidity cuts, there still exists a region where the number of events is larger than $\mathcal{O}(10)$. We also find that conventional triggers can greatly limit the sensitivity of our signal, so we display several relevant kinematical distributions which might aid in the opti…

PhysicsParticle physicsLarge Hadron ColliderPhysics and Astronomy (miscellaneous)Physics beyond the Standard ModelHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaType (model theory)Nuclear physicsHigh Energy Physics - PhenomenologySeesaw mechanismHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryPseudorapidityHiggs bosonHigh Energy Physics::ExperimentNeutrinoEngineering (miscellaneous)The European Physical Journal C
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Soft masses in SUSY SO(10) GUTs with low intermediate scales

2012

The specific shape of the squark, slepton and gaugino mass spectra, if measured with sufficient accuracy, can provide invaluable information not only about the dynamics underpinning their origin at some very high scale such as the unification scale MG, but also about the intermediate scale physics encountered throughout their RGE evolution down to the energy scale accessible for the LHC. In this work, we study general features of the TeV scale soft SUSY breaking parameters stemming from a generic mSugra configuration within certain classes of SUSY SO(10) GUTs with different intermediate symmetries below MG. We show that particular combinations of soft masses show characteristic deviations f…

PhysicsParticle physicsLarge Hadron ColliderSeesaw molecular geometryScale (ratio)High Energy Physics::PhenomenologyGauginoHigh Energy Physics::ExperimentSoft SUSY breakingBoundary value problemSupersymmetrySO(10)
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(g−2)e,μ in an extended inverse type-III seesaw model

2021

There has been a longstanding discrepancy between the experimental measurements of the electron and muon anomalous magnetic moments and their predicted values in the Standard Model. This is particularly relevant in the case of the muon $g\ensuremath{-}2$, which has attracted a remarkable interest in the community after the long-awaited announcement of the first results by the Muon $g\ensuremath{-}2$ collaboration at Fermilab, which confirms a previous measurement by the E821 experiment at Brookhaven and enlarges the statistical significance of the discrepancy, now at $4.2\ensuremath{\sigma}$. In this paper we consider an extension of the inverse type-III seesaw with a pair of vectorlike lep…

PhysicsParticle physicsMuonSeesaw molecular geometryPhysics::Instrumentation and DetectorsInverseHigh Energy Physics::ExperimentElectroweak scaleNeutrinoType (model theory)LeptonStandard ModelPhysical Review D
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