Search results for "Neutrino Mass"

showing 10 items of 53 documents

Accidental stability of dark matter

2013

We propose that dark matter is stable as a consequence of an accidental Z(2) that results from a flavour symmetry group which is the double-cover group of the symmetry group of one of the regular geometric solids. Although model-dependent, the phenomenology resembles that of a generic >inert Higgs> dark matter scheme.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDark matterHigh Energy Physics::Phenomenologyneutrino masses and mixingFOS: Physical sciencesFísicaSymmetry group01 natural sciencesdark matterHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Accidental0103 physical sciencesHiggs boson010306 general physicsPhenomenology (particle physics)flavour symmetry
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Q values of the 76Ge and 100Mo double-beta decays

2008

Abstract Penning trap measurements using mixed beams of 76Ge–76Se and 100Mo–100Ru have been utilized to determine the double-beta decay Q-values of 76Ge and 100Mo with uncertainties less than 200 eV. The value for 76Ge, 2039.04(16) keV is in agreement with the published SMILETRAP value, 2039.006(50) keV. The new value for 100Mo, 3034.40(17) keV is 30 times more precise than the previous literature value, sufficient for the ongoing neutrinoless double-beta decay searches in 100Mo. Moreover, the precise Q-value is used to calculate the phase-space integrals and the experimental nuclear matrix element of double-beta decay.

PhysicsNuclear and High Energy PhysicsParticle physicsDecay schemeQ valuePenning trapDouble-beta decayPenning trapQ-valueBeta decayPhase-space integralNuclear physicsNeutrino massPhase spaceDouble beta decayBeta (plasma physics)Value (mathematics)Physics Letters B
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Testing the Zee-Babu model via neutrino data, lepton flavour violation and direct searches at the LHC

2014

We discuss how the Zee-Babu model can be tested combining information from neutrino data, low-energy experiments and direct searches at the LHC. We update previous analysis in the light of the recent measurement of the neutrino mixing angle $\theta_{13}$, the new MEG limits on $\mu \rightarrow e \gamma$, the lower bounds on doubly-charged scalars coming from LHC data, and, of course, the discovery of a 125 GeV Higgs boson by ATLAS and CMS. In particular, we find that the new singly- and doubly-charged scalars are accessible at the second run of the LHC, yielding different signatures depending on the neutrino hierarchy and on the values of the phases. We also discuss in detail the stability …

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsFlavourHigh Energy Physics::PhenomenologyFOS: Physical sciencesNeutrino masses01 natural sciencesPartícules (Física nuclear)Nuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Lepton flavor violation0103 physical sciencesHiggs bosonGran col·lisionador d'hadrons (França i Suïssa)LHCNeutrino010306 general physicsNeutrino oscillationstability of the potentialLeptonNuclear and Particle Physics Proceedings
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Finding the Higgs boson through supersymmetry

2009

6 pages, 7 figures.-- PACS nrs.: 12.60.Jv; 13.85.Ni; 14.60.Pq; 14.80.Cp.-- ArXiv pre-print available at: http://arxiv.org/abs/0809.1637

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderSupergravity[PACS] Non-standard-model Higgs bosonsElectroweak interactionBosón de HiggsHigh Energy Physics::Phenomenology[PACS] Supersymmetric unified modelsFOS: Physical sciencesFísicaSupersymmetry[PACS] Neutrino mass and mixingSupersymmetry breaking[PACS] Hadron-induced inclusive production with identified hadrons (energy > 10 GeV)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)SupersimetríaHiggs bosonHigh Energy Physics::ExperimentNeutrino oscillationMinimal Supersymmetric Standard Model
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Flavor physics at large tanβwith a binolike lightest supersymmetric particle

2007

12 pages, 7 figures.-- PACS nrs.: 12.60.Jv; 13.25.Hw; 13.35.-r; 95.35.+d.-- ISI Article Identifier: 000247625300053.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0703035

PhysicsNuclear and High Energy PhysicsParticle physicsStandard ModelRelic densityDark matter[PACS] Supersymmetric unified modelsSuperpartnerNeutrino massesSupersymmetryLightest Supersymmetric ParticleStandard ModelNuclear physics[PACS] Hadronic decays of bottom mesonsLepton flavour[PACS] Decays of leptons[PACS] Dark matter (stellar interstellar galactic and cosmological)B mesonNeutrinoFlavorPhysical Review D
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Minimal supergravity radiative effects on the tri-bimaximal neutrino mixing pattern

2007

7 pages, 3 figures.-- PACS nrs.: 14.60.Pq, 12.60.Jv.-- ISI Article Identifier: 000245333000012.-- ArXiv pre-print available at: http://arxiv.org/abs/hep-ph/0606082

PhysicsNuclear and High Energy PhysicsParticle physicsSupergravityHigh Energy Physics::PhenomenologyNumber nonconservation[PACS] Supersymmetric unified modelsFOS: Physical sciencesFísicaWeinberg angleSupersymmetry[PACS] Neutrino mass and mixingMass operator renormalizationSupersymmetry breakingHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Radiative transferSymmetry breakingNeutrinoRight symmetry-breakingMixing (physics)
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Non-standard interactions: Atmospheric versus neutrino factory experiments

2001

We consider the potential of a generic neutrino factory (NUFACT) in probing non-standard neutrino-matter interactions (NSI). We find that the sensitivity to flavour-changing (FC) NSI can be substantially improved with respect to present atmospheric neutrino data, especially at energies higher than approximately 50 GeV, where the effect of the tau mass is small. For example, a 100 GeV NUFACT can probe FC neutrino interactions at the level of few $|\epsilon| < {few} \times 10^{-4}$ at 99 % C.L.

PhysicsParticle physicsAtmospheric neutrinosNuclear and High Energy PhysicsNeutrino mass and mixingNeutrino oscillationsAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyNeutrino factoryFOS: Physical sciencesFísicaHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Neutrino FactoryHigh Energy Physics::ExperimentSensitivity (control systems)Atmospheric neutrinoNeutrino
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A non-resonant dark-side solution to the solar neutrino problem

2001

We re-analyse spin-flavour precession solutions to the solar neutrino problem in the light of the recent SNO CC result as well as the 1258--day Super-Kamiokande data and the upper limit on solar anti-neutrinos. In a self-consistent magneto-hydrodynamics approach the resulting scheme has only 3 effective parameters: $\Delta m^2$, $\mu B_\perp$ and the neutrino mixing angle $\theta$. We show how a rates-only analysis for fixed $\mu B_\perp$ slightly favours spin-flavour precession (SFP) solutions over oscillations (OSC). In addition to the resonant solution (RSFP for short), there is a new non-resonant solution (NRSFP) in the ``dark-side''. Both RSFP and NRSFP lead to flat recoil energy spect…

PhysicsParticle physicsNuclear and High Energy PhysicsNeutrino mass and mixingCosmologiaMagnetic momentNeutrino oscillationsSolar neutrinosHigh Energy Physics::PhenomenologyFOS: Physical sciencesSolar neutrino problemSpectral linePartícules (Física nuclear)Magnetic fieldBohr magnetonNeutrino magnetic momentsymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)symbolsPrecessionHigh Energy Physics::ExperimentNeutrinoMixing (physics)
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Structure and prospects of the simplest SO(10) GUTs

2012

We recapitulate the latest results on the class of the simplest SO(10) grand unified models in which the GUT-scale symmetry breaking is triggered by an adjoint Higgs representation. We argue that the minimal survival approximation traditionally used in the GUT- and seesaw-scale estimates tends to be blind to very interesting parts of the parameter space in which some of the intermediate-scale states necessary for non-supersymmetric unification of the SM gauge couplings can be as light as to leave their imprints in the TeV domain. The stringent minimal-survival-based estimates of the B-L scale are shown to be relaxed by as much as four orders of magnitude, thus admitting for a consistent imp…

PhysicsParticle physicsSO(10)010308 nuclear & particles physicsProton decayHigh Energy Physics::PhenomenologyGrand unification; Neutrino masses; SO(10)Structure (category theory)FOS: Physical sciencesNeutrino massesParameter space01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Seesaw mechanismOrders of magnitude (time)Grand unification0103 physical sciencesHiggs bosonSymmetry breakingSO(10)010306 general physics
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Quark-lepton mass relation and CKM mixing in an A(4) extension of the minimal supersymmetric standard model

2013

An interesting mass relation between down-type quarks and charged leptons has been recently predicted within a supersymmetric SU(3)(c) circle times SU(2)(L) circle times U(1)(Y) model based on the A(4) flavor symmetry. Here we propose a simple extension which provides an adequate full description of the quark sector. By adding a pair of vectorlike up quarks, we show how the CKM entries V-ub, V-cb, V-td and V-ts arise from deviations of the unitarity. We perform an analysis including the most relevant observables in the quark sector, such as oscillations and rare decays of kaons, B-d and B-s mesons. In the lepton sector, the model predicts an inverted hierarchy for the neutrino masses, leadi…

PhysicsQuarkNuclear and High Energy PhysicsParticle physicsMesonUnitarity010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixPhysics beyond the Standard ModelHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaSupersymmetryNeutrino masses01 natural sciencesHigh Energy Physics - PhenomenologySymmetryHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesUp quarkHigh Energy Physics::Experiment010306 general physicsLepton
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