Search results for "Matrix"

showing 10 items of 3205 documents

Predictive flavor symmetries of the neutrino mass matrix.

2007

Here we propose an $A_4$ flavour symmetry model which implies a lower bound on the neutrinoless double beta decay rate, corresponding to an effective mass parameter $M_{ee} \gsim 0.03$ eV, and a direct correlation between the expected magnitude of CP violation in neutrino oscillations and the value of $\sin^2\theta_{13}$, as well as a nearly maximal CP phase $\delta$.

PhysicsParticle physicsHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyFOS: Physical sciencesFísicaMass matrixUpper and lower boundsMonod-Wyman-Changeux modelNuclear physicsHigh Energy Physics - PhenomenologyEffective mass (solid-state physics)High Energy Physics - Phenomenology (hep-ph)Double beta decayCP violationHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationPhysical review letters
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Neutrino masses in the Standard Model effective field theory

2021

We would like to thank Xiao-Dong Ma for help in understanding some of the computations in Ref. [27]. We would like to thank Guilherme Guedes, Maria Ramos, Jose Santiago, and Arcadi Santamaria for useful discussions. M. C. is supported by the Spanish MINECO under the Ramon y Cajal program and partially by the Ministry of Science and Innovation under Grant No. FPA201678220-C3-1/3-P (FEDER), Spanish State Research Agency (Agencia Estatal de Investigacion) under Grant No. PID2019-106087 GB-C21/C22 (10.13039/501100011033) as well as by the Junta de Andalucia Grants No. FQM 101 and No. A-FQM-211-UGR18, and No. P18-FR-4314 (FEDER). A. T. is supported by the Generalitat Valenciana under Grant No. P…

PhysicsParticle physicsHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesOrder (ring theory)Mass matrixLepton numberHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)Effective field theoryHigh Energy Physics::ExperimentNeutrinoLeptonPhysical Review D
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A flavour physics scenario for the 750 GeV diphoton anomaly

2016

A simple variant of a realistic flavor symmetry scheme for fermion masses and mixings provides a possible interpretation of the diphoton anomaly as an electroweak singlet ``flavon.'' The existence of TeV scale vectorlike T-quarks required to provide adequate values for Cabibbo-Kobayashi-Maskawa (CKM) parameters can also naturally account for the diphoton anomaly. Correlations between ${V}_{ub}$ and ${V}_{cb}$ with the vectorlike T-quark mass can be predicted. Should the diphoton anomaly survive in a future run, our proposed interpretation can also be tested in upcoming B and LHC studies.

PhysicsParticle physicsLarge Hadron Collider010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixPhysics beyond the Standard ModelHigh Energy Physics::LatticeElectroweak interactionHigh Energy Physics::PhenomenologyFOS: Physical sciencesFermion01 natural sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHigh Energy Physics::ExperimentSimple variant010306 general physicsFlavorComputer Science::Databases
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Semileptonic decays of B(*) , D(*) into νl and pseudoscalar or vector mesons

2018

We perform a study of the ${B}^{(*)}$, ${D}^{(*)}$ semileptonic decays, using a different method than in conventional approaches, where the matrix elements of the weak operators are evaluated and a detailed spin-angular momentum algebra is performed to obtain very simple expressions at the end for the different decay modes. Using only one experimental decay rate in the $B$ or $D$ sectors, the rates for the rest of decay modes are predicted and they are in good agreement with experiment. Some discrepancies are observed in the $\ensuremath{\tau}$ decay mode for which we find an explanation. We perform evaluations for ${B}^{*}$ and ${D}^{*}$ decay rates that can be used in future measurements,…

PhysicsParticle physicsMeson010308 nuclear & particles physics01 natural sciencesPseudoscalar mesonMomentumPseudoscalarMatrix (mathematics)0103 physical sciencesHigh Energy Physics::ExperimentVector mesonAlgebra over a field010306 general physicsPhysical Review D
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Colloquium: Time-reversal violation with quantum-entangled B mesons

2014

Symmetry transformations have been proven a bedrock tool for understanding the nature of particle interactions, formulating and testing fundamental theories. Based on the up to now unbroken CPT symmetry, the violation of the CP symmetry between matter and antimatter by weak interactions, discovered in the decay of kaons in 1964 and observed more recently in 2001 in B mesons, strongly suggests that the behavior of these particles under weak interactions must also be asymmetric under time reversal T. However, until the recent years there has not been a direct detection of the expected time-reversal violation in the time evolution of any system. This Colloquium examines the field of time-rever…

PhysicsParticle physicsMesonCabibbo–Kobayashi–Maskawa matrixmedia_common.quotation_subjectFOS: Physical sciencesGeneral Physics and AstronomyFísicaQuantum entanglementAsymmetrySymmetry (physics)B-factoryHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CP violationHigh Energy Physics::ExperimentSymmetry breakingmedia_common
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Chiral symmetry amplitudes in the S-wave isoscalar and isovector channels and the σ, f[sub 0](980), a[sub 0](980) scalar mesons

1998

We use a nonperturbative approach which combines coupled channel Lippmann Schwinger equations with meson-meson potentials provided by the lowest order chiral Lagrangian. By means of one parameter, a cut off in the momentum of the loop integrals, which results of the order of 1 GeV, we obtain singularities in the S-wave amplitudes corresponding to the σ, f0 and a0 resonances. The ππ→ππ, ππ→KK phase shifts and inelasticities in the T=0 scalar channel are well reproduced as well as the π0η and KK mass distributions in the T=1 channel. Furthermore, the total and partial decay widths of the f0 and a0 resonances are properly reproduced. The results seem to indicate that chiral symmetry constraint…

PhysicsParticle physicsMesonIsovectorUnitarityHigh Energy Physics::LatticeIsoscalarHigh Energy Physics::PhenomenologyScalar (mathematics)Lippmann–Schwinger equationMomentumQuantum electrodynamicsHigh Energy Physics::ExperimentS-matrixAIP Conference Proceedings
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Search for heavy neutrinos in \(\pi ^{ + } \to \mu ^{ + }\nu \) decay and status of lepton universality test in the PIENU experiment

2019

International audience; In the present work of the PIENU experiment, heavy neutrinos were sought in pion decays \(\pi ^{ + } \to \mu ^{ + }\nu \). No evidence for extra peak was found in the muon kinetic energy spectrum and 90% confidence level upper limits were set on the neutrino mixing matrix \(|U_{\mu i}|^{2}\) in the mass range of 15.7 to 33.8 MeV/c^2, improving an order of magnitude over previous experiments. Current status of lepton universality test is also reported.

PhysicsParticle physicsMuonpi+ --> muon+ neutrinopi: decayneutrino: heavy: search forUniversality (philosophy)Pontecorvo–Maki–Nakagawa–Sakata matrixkineticenergy spectrumKinetic energyPion[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentNeutrinoneutrino: mixingOrder of magnitudeParticle Physics - ExperimentLeptonexperimental resultslepton: universality
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A Theoretical Prediction of the Bs-Meson Lifetime Difference

2000

We present the results of a quenched lattice calculation of the operator matrix elements relevant for predicting the Bs width difference. Our main result is (\Delta\Gamma_Bs/\Gamma_Bs)= (4.7 +/- 1.5 +/- 1.6) 10^(-2), obtained from the ratio of matrix elements, R(m_b)=/=-0.93(3)^(+0.00)_(-0.01). R(m_b) was evaluated from the two relevant B-parameters, B_S^{MSbar}(m_b)=0.86(2)^(+0.02)_(-0.03) and B_Bs^{MSbar}(m_b) = 0.91(3)^(+0.00)_(-0.06), which we computed in our simulation.

PhysicsParticle physicsNONPERTURBATIVE RENORMALIZATIONPhysics and Astronomy (miscellaneous)MesonHigh Energy Physics - Lattice (hep-lat)Analytical chemistryFOS: Physical sciencesPartícules (Física nuclear)Settore FIS/02 - Fisica Teorica Modelli e Metodi MatematiciHigh Energy Physics - PhenomenologyOperator matrixMATRIX-ELEMENTSHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)Lattice (order)Engineering (miscellaneous)QCD CORRECTIONSTO-LEADING ORDER
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Neutrino oscillations and the seesaw origin of neutrino mass

2016

The historical discovery of neutrino oscillations using solar and atmospheric neutrinos, and subsequent accelerator and reactor studies, has brought neutrino physics to the precision era. We note that CP effects in oscillation phenomena could be difficult to extract in the presence of unitarity violation. As a result upcoming dedicated leptonic CP violation studies should take into account the non-unitarity of the lepton mixing matrix. Restricting non-unitarity will shed light on the seesaw scale, and thereby guide us towards the new physics responsible for neutrino mass generation.

PhysicsParticle physicsNuclear and High Energy Physics010308 nuclear & particles physicsSolar neutrinoHigh Energy Physics::PhenomenologyPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical sciencesSolar neutrino problem01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Seesaw molecular geometry0103 physical sciencesCP violationMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillation
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Genuine and Matter-induced Components of the CPV Asymmetry for Neutrino Oscillations

2019

These results represent the solution for the historical problem of the contamination by matter effects on the CPV Asymmetry for neutrino oscillations. Vacuum is CPT-symmetric and matter is T-symmetric, the goal is accomplished by using this guiding principle. Independent of the theoretical framework for the dynamics of the active neutrino flavors, we prove the Disentanglement Theorem A(CP)=A(CP, T)+A(CP, CPT) for the experimental CPV Asymmetry, with A(CP, T) genuine T-odd and A(CP, CPT) fake CPT-odd. For the effective Hamiltonian written as the sum of free mass propagation plus the matter potential for electron-neutrinos, the two components have definite parities under the baseline L, the m…

PhysicsParticle physicsOscillationmedia_common.quotation_subjectHigh Energy Physics::PhenomenologyZero (complex analysis)FOS: Physical sciencesAsymmetryHigh Energy Physics - Phenomenologysymbols.namesakeMatrix (mathematics)High Energy Physics - Phenomenology (hep-ph)symbolsHigh Energy Physics::ExperimentNeutrinoHamiltonian (quantum mechanics)Neutrino oscillationSign (mathematics)media_common
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