Search results for "PMNS"

showing 5 items of 5 documents

Non-Unitarity of the lepton mixing matrix at the European spallation source

2022

If neutrinos get mass through the exchange of lepton mediators, as in seesaw schemes, the neutrino appearance probabilities in oscillation experiments are modified due to effective nonunitarity of the lepton mixing matrix. This also leads to new CP phases and an ambiguity in underpinning the ''conventional'' phase of the three-neutrino paradigm. We study the CP sensitivities of various setups based at the European spallation source neutrino super-beam (ESSnuSB) experiment in the presence of nonunitarity. We also examine its potential in constraining the associated new physics parameters. Moreover, we show how the combination of DUNE and ESSnuSB can help further improve the sensitivities on …

PMNS matrixPhysics::Instrumentation and Detectorsnew physicsHigh Energy Physics::Phenomenologyphase: CPFOS: Physical scienceslepton: mixingneutrino: mixing angleHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)ESSnuSB[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]CP: violation[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::Experimentneutrino: oscillationunitarity: violation
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A Comprehensive Mechanism Reproducing the Mass and Mixing Parameters of Quarks and Leptons

2013

It is shown that if, from the starting point of a universal rank-one mass matrix long favored by phenomenologists, one adds the assumption that it rotates (changes its orientation in generation space) with changing scale, one can reproduce, in terms of only six real parameters, all the 16 mass ratios and mixing parameters of quarks and leptons. Of these 16 quantities so reproduced, 10 for which data exist for direct comparison (i.e. the CKM elements including the CP-violating phase, the angles theta(12), theta(13), theta(23) in nu-oscillation, and the masses m(c), m(mu), m(e)) agree well with experiment, mostly to within experimental errors; four others (m(s), m(u), m(d), m(nu 2)), the expe…

Quantum chromodynamicsPhysicsQuarkNuclear and High Energy PhysicsParticle physicsPMNS matrixCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesOrder (ring theory)Astronomy and AstrophysicsMass matrixAtomic and Molecular Physics and OpticsOrientation (vector space)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CKM matrixFermion massesHigh Energy Physics::ExperimentCP phaseNeutrinoLepton
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The Cabibbo angle as a universal seed for quark and lepton mixings

2015

A model-independent ansatz to describe lepton and quark mixing in a unified way is suggested based upon the Cabibbo angle. In our framework neutrinos mix in a "Bi-Large" fashion, while the charged leptons mix as the "down-type" quarks do. In addition to the standard Wolfenstein parameters (lambda, A) two other free parameters are needed to specify the physical lepton mixing matrix. Through this simple assumption one makes specific predictions for the atmospheric angle as well as leptonic CP violation in good agreement with current observations.

QuarkNuclear and High Energy PhysicsParticle physicsPMNS matrixPhysics beyond the Standard ModelPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical sciencesHigh Energy Physics - Phenomenology (hep-ph)ddc:530Mixing (physics)PhysicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::PhenomenologyFísicaBi-Large mixinglcsh:QC1-999High Energy Physics - PhenomenologyCKM matrixCabibbo angleCP violationHigh Energy Physics::ExperimentNeutrinoNeutrino mixingWolfenstein parameterlcsh:PhysicsLepton
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Search for Electron Antineutrino Appearance in a Long-baseline Muon Antineutrino Beam

2020

Electron antineutrino appearance is measured by the T2K experiment in an accelerator-produced antineutrino beam, using additional neutrino beam operation to constrain parameters of the Pontecorvo-Maki-Nakagawa-Sakata (PMNS) mixing matrix. T2K observes 15 candidate electron antineutrino events with a background expectation of 9.3 events. Including information from the kinematic distribution of observed events, the hypothesis of no electron antineutrino appearance is disfavored with a significance of 2.40 σ and no discrepancy between data and PMNS predictions is found. A complementary analysis that introduces an additional free parameter which allows non-PMNS values of electron neutrino and a…

muon antineutrino beamGeneral Physics and Astronomyantineutrino/mu: secondary beamKAMIOKANDEantineutrino/e: particle identification01 natural sciences09 EngineeringHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)secondary beam [neutrino/mu][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]neutrino/e: particle identificationQCPhysics02 Physical SciencesPhysicsJ-PARC LabT2K experimentelectron antineutrinoT2K CollaborationkinematicsPhysical SciencesParticle Physics - ExperimentT2K experiment in an accelerator-producedGeneral Physics530 PhysicsPhysics MultidisciplinaryFOS: Physical sciencesparticle identification [antineutrino/e]Neutrino beamsecondary beam [antineutrino/mu]530Physics::GeophysicsNuclear physics0103 physical sciencesmixingddc:530010306 general physics01 Mathematical SciencesMuonScience & Technologyparticle identification [neutrino/e]hep-exbackgroundHigh Energy Physics - Experiment; High Energy Physics - Experimentneutrino/mu: secondary beamantineutrino: oscillationoscillation [antineutrino]Elementary Particles and FieldsHigh Energy Physics::ExperimentPMNSElectron neutrinoBeam (structure)Free parameterexperimental results
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Neutriinojen ja kvarkkien sekoitusmatriisien välinen yhteys

2012

In this thesis relations between neutrino mixing matrix and quark mixing matrix are studied. The focus of the analysis is on two simple cases. In the first case it is assumed that the left matrix that diagonalizes the mass matrix of charged leptons and the corresponding matrix of down quarks are equal. In the second case it is likewise assumed that the corresponding diagonalizing matrices of neutrinos and up quarks are equal. First, theoretical concepts related to the mixing of quarks and especially to the mixing of neutrinos are presented. These are e.g. fermion mass generation in the Standard Model, Majorana masses of neutrinos and the so-called seesaw mechanism. Regarding experiments, ne…

neutriinosymmetriamassatermikvarkitneutriinotmassamatriisineutriinofysiikkakvarkkisekoitusmatriisisekoittuminenCKMmassateoreettinen fysiikkaQLCfysiikkaPMNSmatriisitMajorana
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