Search results for " neutrinos"

showing 10 items of 140 documents

Update on decaying and annihilating heavy dark matter with the 6-year IceCube HESE data

2019

In view of the IceCube's 6-year high-energy starting events (HESE) sample, we revisit the possibility that the updated data may be better explained by a combination of neutrino fluxes from dark matter decay and an isotropic astrophysical power-law than purely by the latter. We find that the combined two-component flux qualitatively improves the fit to the observed data over a purely astrophysical one, and discuss how these updated fits compare against a similar analysis done with the 4-year HESE data. We also update fits involving dark matter decay via multiple channels, without any contribution from the astrophysical flux. We find that a DM-only explanation is not excluded by neutrino data…

PhysicsHigh Energy Astrophysical Phenomena (astro-ph.HE)dark matter theoryultra high energy photons and neutrinos010308 nuclear & particles physicsIsotropyDark matterFOS: Physical sciencesAstronomy and AstrophysicsAstrophysics01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)13. Climate action0103 physical sciencesNeutrinoAstrophysics - High Energy Astrophysical Phenomena
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Probing neutrino magnetic moments at the Spallation Neutron Source facility

2015

24 pages.- 8 figures

PhysicsNuclear and High Energy PhysicsNeutral currentGauge theoryPhysics beyond the Standard ModelFOS: Physical sciencesFísicaContext (language use)Lepton numberElectromagnetic propertiesStandard ModelNuclear physicsMAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)lepton numberNeutrinoSpallation Neutron SourceMajorana neutrinos
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Energy-independent new physics in the flavour ratios of high-energy astrophysical neutrinos

2010

We have studied the consequences of breaking the CPT symmetry in the neutrino sector, using the expected high-energy neutrino flux from distant cosmological sources such as active galaxies. For this purpose we have assumed three different hypotheses for the neutrino production model, characterised by the flavour fluxes at production phi(0)(e) : phi(0)(mu) : phi(0)(tau) = 1 : 2 : 0, 0 : 1 : 0, and 1 : 0 : 0, and studied the theoretical and experimental expectations for the muon-neutrino flux at Earth, phi(mu), and for the flavour ratios at Earth, R = phi(mu)/phi(e) and S = phi(tau)/phi(mu). CPT violation (CPTV) has been implemented by adding an energy-independent term to the standard neutrin…

PhysicsNuclear and High Energy PhysicsParticle physicsActive galactic nucleusCPT symmetryPhysics beyond the Standard ModelFísicaFOS: Physical sciencesSeparable spacesymbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Astrophysical neutrinossymbolsLarge deviations theoryCPT violationNeutrinoHamiltonian (quantum mechanics)Neutrino oscillation
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Flavour-violating charged lepton decays in seesaw-type models

1994

Analytic expressions of lepton-flavour- and lepton-number-violating decays of charged leptons are derived in the context of general $SU(2)_L\otimes U(1)_Y$ seesaw scenarios that are motivated by grand unified theories (GUT's) or superstring models, in which left-handed and/or right-handed neutral singlets are present. Possible constraints imposed by cosmology and low-energy data are briefly discussed. The violation of the decoupling theorem in flavour-dependent graphs due to the presence of heavy neutral leptons of Dirac or Majorana nature is emphasized. Numerical estimates reveal that the decays $\tau^-\to e^-e^-e^+$ or $\tau^-\to e^-\mu^-\mu^+$ can be as large as $\sim 10^{-6}$, which may…

PhysicsNuclear and High Energy PhysicsParticle physicsDirac (video compression format)High Energy Physics::PhenomenologyFOS: Physical sciencesSuperstring theoryContext (language use)Lepton flavour violation ; seesaw ; singlet Majorana/Dirac neutrinosType (model theory)CosmologyHigh Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometryHigh Energy Physics::ExperimentLepton
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Short-range mechanisms of neutrinoless double beta decay at the LHC

2013

Lepton number violation (LNV) mediated by short- range operators can manifest itself in both neutrinoless double beta decay (0 nu beta beta) and in processes with same- sign dilepton final states at the LHC. We derive limits from existing LHC data at root s = 8 TeV and compare the discovery potential of the forthcoming root s = 14 TeV phase of the LHC with the sensitivity of current and future 0 nu beta beta decay experiments, assuming the short-range part of the 0 nu beta beta decay amplitude dominates. We focus on the first of two possible topologies triggered by one fermion and two bosons in the intermediate state. In all cases, except for the pure leptoquark mechanism, the LHC will be m…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísica01 natural sciences7. Clean energyHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decay0103 physical sciencesHigh Energy Physics::ExperimentLepton number010306 general physicsHumanitiesMajorana neutrinosPhysical Review D
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LHC dijet constraints on double beta decay

2015

13 pages.- 5 figures

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhysics beyond the Standard ModelScalar (mathematics)High Energy Physics::PhenomenologyFísicaFOS: Physical sciencesLepton numberNuclear physicsDiquarkHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayLepton numberHigh Energy Physics::ExperimentNeutrinoMajorana neutrinosBoson
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Neff versus the lightest neutrino mass

2016

AbstractWithin the framework of low-scale Type I seesaw models with two and three extra sterile neutrinos we evaluate the production of the sterile states in the Early Universe. We explore the full parameter space and find that in the model with two extra states both of them reach thermal equilibrium with the primordial plasma. In the model with three sterile neutrinos, if the lightest active neutrino mass is below O(10−3eV) one sterile neutrino might not thermalize, while the other two always reach thermalization. Applying constrains from both extra radiation at BBN and CMB, and the dark matter allowed abundance, we show that the spectra of heavier states are severely restricted in the mas…

PhysicsNuclear and High Energy PhysicsParticle physicsSterile neutrino010308 nuclear & particles physicsSolar neutrinoHigh Energy Physics::PhenomenologyNeutrino decouplingSolar neutrino problem01 natural sciencesseesaw modelCosmic neutrino backgroundNuclear physicssterile neutrinos0103 physical sciencesMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationNuclear and Particle Physics Proceedings
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The response of (95,97)Mo to supernova neutrinos

2011

Knowledge about nuclear responses to neutrinos is essential for both astrophysical applications and studies of neutrino properties. We perform in this paper calculations of the cross sections for neutral-current neutrino scattering off the odd A = 95,97 Mo isotopes for energies appropriate for the detection of supernova neutrinos. Both the incoherent and coherent contributions to the cross sections are evaluated. The prominently contributing nuclear final states are identified and analysed. We employ the microscopic quasiparticle-phonon model (MQPM) to construct the wave functions of the initial and final nuclear states. The response of the aforementioned nuclei to supernova neutrinos are c…

PhysicsNuclear and High Energy PhysicsParticle physicsneutrino-nucleus scatteringIsotopedetectorAstrophysics::High Energy Astrophysical PhenomenaType II supernovamicroscopic quasiparticle-phonon modelNeutrino scatteringNuclear physicsCosmic neutrino backgroundSupernovaAbstract knowledgeMeasurements of neutrino speedmassNeutrinosupernova neutrinos
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Search for heavy neutrinos in K + → μ + ν μ decays

2017

The NA62 experiment recorded a large sample of K+→μ+νμ decays in 2007. A peak search has been performed in the reconstructed missing mass spectrum. In the absence of a signal, limits in the range 2×10−6 to 10−5 have been set on the squared mixing matrix element |Uμ4|2 between muon and heavy neutrino states, for heavy neutrino masses in the range 300–375 MeV/ c2 . The result extends the range of masses for which upper limits have been set on the value of |Uμ4|2 in previous production search experiments.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Particle physicsMuon010308 nuclear & particles physicsPhysics beyond the Standard ModelHeavy neutrinoNA62 experiment01 natural scienceslcsh:QC1-999Heavy neutrinos; Kaon decays; Nuclear and High Energy PhysicsNuclear physicsKaon decayHeavy neutrinos0103 physical sciencesMass spectrumKaon decaysNeutrinoHeavy neutrino010306 general physicslcsh:PhysicsMixing (physics)
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On the description of non-unitary neutrino mixing

2015

28 pages.- 8 figures.- typos corrected.- modified bounds on non-unitarity parameters.- new figs 3 and 4

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsUnitarityPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyPontecorvo–Maki–Nakagawa–Sakata matrixFísicaFOS: Physical sciencesDouble beta decayHigh Energy Physics - ExperimentStandard Model (mathematical formulation)High Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Heavy majorana neutrinosMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillation
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