Search results for "Matrix"

showing 10 items of 3205 documents

DYNAMICALLY GENERATED RESONANCES IN THE CHIRAL UNITARY APPROACH TO MESON BARYON INTERACTION

2004

In this talk we report on the use of a chiral unitary approach for the interaction of the octets of meson and baryon and the octet of mesons with the decuplet of baryons. Two octets of $J^{\pi}=1/2^-$ baryon states and a singlet are generated dynamically in the first case, resulting in the case of strangeness $S=-1$ in two poles of the scattering matrix close to the nominal $\Lambda(1405)$ resonance. In the second case many resonances are also generated, among them an exotic baryon with S=1 corresponding to a $\Delta K$ resonance. We make suggestions of experiments which could show evidence for the existence of these states.

PhysicsNuclear and High Energy PhysicsParticle physicsOctetMesonHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaAstronomy and AstrophysicsStrangenessLambdaUnitary stateAtomic and Molecular Physics and OpticsBaryonHigh Energy Physics - PhenomenologyMatrix (mathematics)High Energy Physics - Phenomenology (hep-ph)Exotic baryonHigh Energy Physics::ExperimentNuclear ExperimentInternational Journal of Modern Physics A
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CP violation and neutrino oscillations

2007

We review the basic mechanisms of neutrino mass generation and the corresponding structure of the lepton mixing matrix. We summarize the status of three-neutrino oscillation parameters as determined from current observations, using state-of-the-art solar and atmospheric neutrino fluxes, as well as latest experimental data as of September 2007. We also comment on recent attempts to account for these results and to understand flavour from first principles. We discuss extensively the prospects for probing the strength of CP violation in two near term accelerator neutrino oscillation experiments, T2K and NOvA, as well as possible extensions such as T2KK and a second large off-axis detector near…

PhysicsNuclear and High Energy PhysicsParticle physicsOscillationPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyPontecorvo–Maki–Nakagawa–Sakata matrixFOS: Physical sciencesFísicaMAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Double beta decayLeptogenesisCP violationHigh Energy Physics::ExperimentNeutrinoNeutrino oscillation
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Constraining Majorana neutrino electromagnetic properties from the LMA-MSW solution of the solar neutrino problem

2002

In this paper we use solar neutrino data to derive stringent bounds on Majorana neutrino transition moments (TMs). Should such be present, they would contribute to the neutrino--electron scattering cross section and hence alter the signal observed in Super-Kamiokande. Motivated by the growing robustness of the LMA-MSW solution of the solar neutrino problem indicated by recent data, and also by the prospects of its possible confirmation at KamLAND, we assume the validity of this solution, and we constrain neutrino TMs by using the latest global solar neutrino data. We find that all elements of the TM matrix can be bounded at the same time. Furthermore, we show how reactor data play a complem…

PhysicsNuclear and High Energy PhysicsParticle physicsOscillationSolar neutrinoHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesSolar neutrino problemMatrix (mathematics)MAJORANAHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentNeutrinoBorexinoOrder of magnitude
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Neutrino mixing with revamped A(4) flavor symmetry

2013

We suggest a minimal extension of the simplest A(4) flavor model that can induce a nonzero theta(13) value, as required by recent neutrino oscillation data from reactors and accelerators. The predicted correlation between the atmospheric mixing angle theta(23) and the magnitude of theta(13) leads to an allowed region substantially smaller than indicated by neutrino-oscillation global fits. Moreover, the scheme correlates CP violation in neutrino oscillations with the octant of the atmospheric mixing parameter theta(23) in such a way that, for example, maximal mixing necessarily violates CP. We briefly comment on other phenomenological features of the model.

PhysicsNuclear and High Energy PhysicsParticle physicsOscillations010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísica01 natural sciencesNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Mass Matrix0103 physical sciencesHigh Energy Physics::ExperimentNeutrino010306 general physicsNeutrino oscillationMixing (physics)
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Clues for the existence of twoK1(1270)resonances

2007

The axial-vector meson ${K}_{1}(1270)$ was studied within the chiral unitary approach, where it was shown that it has a two-pole structure. We reanalyze the high-statistics WA3 experiment ${K}^{\ensuremath{-}}p\ensuremath{\rightarrow}{K}^{\ensuremath{-}}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}p$ at 63 GeV, which established the existence of both ${K}_{1}(1270)$ and ${K}_{1}(1400)$, and we show that it clearly favors our two-pole interpretation. We also reanalyze the traditional $K$-matrix interpretation of the WA3 data and find that the good fit of the data obtained there comes from large cancellations of terms of unclear physical interpretation.

PhysicsNuclear and High Energy PhysicsParticle physicsParticle decayChiral perturbation theoryPair productionBethe–Salpeter equationMesonUnitarityK matrixInterpretation (model theory)Physical Review D
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Exclusive measurements of b → sγ transition rate and photon energy spectrum

2012

We use 429  fb^(-1) of e^+e^- collision data collected at the Υ(4S) resonance with the BABAR detector to measure the radiative transition rate of b→sγ with a sum of 38 exclusive final states. The inclusive branching fraction with a minimum photon energy of 1.9 GeV is found to be B(B → X_sγ)=(3.29±0.19±0.48)×10+(-4) where the first uncertainty is statistical and the second is systematic. We also measure the first and second moments of the photon energy spectrum and extract the best-fit values for the heavy-quark parameters, m_b and μ_π^2, in the kinetic and shape function models.

PhysicsNuclear and High Energy PhysicsParticle physicsPhoton010308 nuclear & particles physicsBranching fractionElectron–positron annihilationPhoton energyKinetic energyTransition rate matrix01 natural sciencesMeasure (mathematics)Resonance (particle physics)Nuclear physics0103 physical sciencesHigh Energy Physics::Experiment010306 general physics
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Incoherent pion photoproduction on the deuteron with polarization observables II: Influence of final state rescattering

2005

Incoherent pion photoproduction on the deuteron is studied for photon energies from threshold up to 1 GeV with special emphasis on polarization observables. The elementary $\gamma N\to\pi N$ amplitude is taken from the MAID model. The influence of final state interactions on total and semi-exclusive cross sections $\vec d(\vec\gamma,\pi)NN$ is investigated by including complete rescattering in the final $NN$- and $\pi N$-subsystems. For charged pion-production the influence of $NN$-rescattering is moderate whereas $\pi N$-rescattering is almost negligible. Much stronger influences of $NN$-rescattering are seen in neutral pion production, which is due to the elimination of a significant spur…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonNuclear Theorymedia_common.quotation_subjectNuclear TheoryFOS: Physical sciencesFew-body systemsPolarization (waves)AsymmetryNuclear physicsNuclear Theory (nucl-th)PionAmplitudeDeuteriumNuclear Experimentmedia_commonS-matrix
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Heavy neutrino mixing and single production at linear collider

1997

We study the single production of heavy neutrinos via the processes $e^-e^+ \to \nu N$ and $e^-\gamma \to W^- N$ at future linear colliders. As a base of our considerations we take a wide class of models, both with vanishing and non-vanishing left-handed Majorana neutrino mass matrix $m_L$. We perform a model independent analyses of the existing experimental data and find connections between the characteristic of heavy neutrinos (masses, mixings, CP eigenvalues) and the $m_L$ parameters. We show that with the present experimental constraints heavy neutrino masses almost up to the collision energy can be tested in the future experiments.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and Detectors010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyFOS: Physical sciencesMass matrix01 natural sciences7. Clean energylaw.inventionBase (group theory)High Energy Physics - PhenomenologyMAJORANAHigh Energy Physics - Phenomenology (hep-ph)law0103 physical sciencesHigh Energy Physics::ExperimentProduction (computer science)Neutrino010306 general physicsColliderEigenvalues and eigenvectorsMixing (physics)Physics Letters B
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Gluonic contributions in the chiral hyperbag

1990

Abstract We incorporate into a non-perturbative chiral bag model scheme the gluons and the η' in a perturbative fashion. We analyze in this context the proton matrix element for the flavor singlet axial current, where due account is taken of the anomaly, and the delta-nucleon mass difference. Our results show that the contribution due to the gluons is significant for large bag radii and that they are crucial in order to establish the Cheshire cat principle.

PhysicsNuclear and High Energy PhysicsParticle physicsQuantization (physics)High Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryAxial currentMatrix elementSinglet stateNuclear ExperimentGluonNuclear Physics A
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Implications of a Rotating Mass Matrix

2001

The fermion mass matrix, in addition to having eigenvalues (masses) which run, also changes its orientation (rotates) with changing energy scales. This means that its eigenstates at one scale will no longer be eigenstates at another scale, leading to effects where fermions of different flavours can ``transmute'' into one another. In this paper, the implications of a rotating mass matrix are analysed and possible transmuation effects are investigated both in the Standard Model (SM) and in the so-called Dualized Standard Model (DSM) that we advocate, arriving at the conclusion that some transmutational decays such as $\psi \longrightarrow \mu \tau$, $\Upsilon \longrightarrow \mu \tau$ or $\pi…

PhysicsNuclear and High Energy PhysicsParticle physicsScale (ratio)Electron–positron annihilationFísicaFOS: Physical sciencesFermionMass matrixStandard ModelOrientation (vector space)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Energy (signal processing)Eigenvalues and eigenvectors
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