Search results for "Matrix"

showing 10 items of 3205 documents

Y(3940),Z(3930), and theX(4160)as dynamically generated resonances from the vector-vector interaction

2009

We apply a unitary approach together with a set of hidden‐gauge Lagrangians to study the vector‐vector interaction. Concretely, we focus on the sector with quantum numbers charm C = 0 and strangeness S = 0 in the region around 4000 MeV. We get five poles, three of which could be identified with the Y(3940), Z(3930) and X(4160). These poles appear with quantum numbers I = 0 and JPC = 0++,2++ and 2++, respectively, and can be considered as hadronic molecules made of D*D*, Ds*Ds*, decaying to a pair of light vectors, light‐heavy vector or pseudoscalar‐pseudoscalar.

PhysicsNuclear and High Energy PhysicsParticle physicsMeson010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHadronVector meson dominanceStrangenessQuantum number01 natural sciences0103 physical sciencesBound stateHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsS-matrixSpin-½Physical Review D
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Measurements of |Vcb|, form factors and branching fractions in the decays → ℓ and → ℓ

1997

Two samples of exclusive semileptonic decays, 579 B0 -> D*+l-νl events and 261 B0 -> D+l-νl events, are selected from approximately 3.9 million hadronic Z decays collected by the ALEPH detector at LEP. From the reconstructed differential decay rate of each sample, the product of the hadronic form factor F(ω) at zero recoil of the D(*)+ meson and the CKM matrix element Vcb are measured to be FD*+ (1) Vcb = (31.9 +/- 1.8stat +/- 1.9syst) × 10-3,FD+ (1) Vcb = (27.8 +/- 6.8stat +/- 6.5syst) × 10-3. The ratio of the form factorsFD+ (1) and FD*+ (1) is measured to beFD+ (1)/FD*+ (1) = 0.87 +/- 0.22stat +/- 0.21syst. A value of Vcb is extracted from the two samples, using theoretical constraints o…

PhysicsNuclear and High Energy PhysicsParticle physicsMesonCabibbo–Kobayashi–Maskawa matrixElectron–positron annihilationHigh Energy Physics::PhenomenologyHadronCurvatureSpectral lineALEPH ExperimentRecoilHigh Energy Physics::ExperimentAtomic physicsALEPH experimentPhysics Letters B
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Minimal Flavour Violation and Multi-Higgs Models

2010

We propose an extension of the hypothesis of Minimal Flavour Violation (MFV) to general multi-Higgs models without the assumption of Natural Flavour Conservation (NFC) in the Higgs sector. We study in detail under what conditions the neutral Higgs couplings are only functions of V-CKM and propose a MFV expansion for the neutral Higgs couplings to fermions

PhysicsNuclear and High Energy PhysicsParticle physicsMinimal Flavour Violation010308 nuclear & particles physicsCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyFísicaFOS: Physical sciencesFCNCFermion01 natural sciencesHiggs sectorFlavour symmetriesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Multi-Higgs models0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsParticle Physics - Phenomenology
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A large magnetic detector for the neutrino factory

2000

Abstract The physics opportunities of the neutrino factory have been the subject of a number of recent studies. It was shown that sensitive measurements of the angle θ 13 , of MSW effects, and of the sign of the atmospheric mass difference Δ m 23 2 are possible, and even CP violation in the neutrino mixing matrix may be within reach. The focus of interest is the oscillation ν e →ν μ , which leads in the well-defined neutrino beam of the neutrino factory to ‘wrong-sign’ muon events. In this paper, we show that a large magnetic detector will be capable of detecting with high efficiency and small backgrounds such wrong-sign muon events. We present a conceptual design of the apparatus and its p…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonPhysics::Instrumentation and DetectorsPontecorvo–Maki–Nakagawa–Sakata matrixSolar neutrino problemNuclear physicsNeutrino detectorMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrino FactoryNeutrinoNeutrino oscillationInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Flavour constraints on multi-Higgs-doublet models: Yukawa alignment

2010

6 páginas, 3 figuras, 1 tabla.-- Talk given in the "Third Workshop on Theory, Phenomenology and Experiments in Heavy Flavour Physics" (Capri, 5-7 July 2010).

PhysicsNuclear and High Energy PhysicsParticle physicsNeutral currentCabibbo–Kobayashi–Maskawa matrixHigh Energy Physics::LatticeFlavourHigh Energy Physics::PhenomenologyYukawa potentialFOS: Physical sciencesFermionAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Higgs bosonCP violationHigh Energy Physics::ExperimentPhenomenology (particle physics)
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Precision thrust cumulant moments atN3LL

2012

We consider cumulant moments (cumulants) of the thrust distribution using predictions of the full spectrum for thrust including O(alpha_s^3) fixed order results, resummation of singular N^3LL logarithmic contributions, and a class of leading power corrections in a renormalon-free scheme. From a global fit to the first thrust moment we extract the strong coupling and the leading power correction matrix element Omega_1. We obtain alpha_s(m_Z) = 0.1141 \pm (0.0004)_exp \pm (0.0014)_hadr \pm (0.0007)_pert, where the 1-sigma uncertainties are experimental, from hadronization (related to Omega_1) and perturbative, respectively, and Omega_1 = 0.372 \pm (0.044)_exp \pm (0.039)_pert GeV. The n-th th…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theory010308 nuclear & particles physicsElectron–positron annihilationFOS: Physical sciencesOrder (ring theory)01 natural sciencesOmegaHigh Energy Physics - ExperimentNuclear Theory (nucl-th)CombinatoricsHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)Power correctionHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesStrong couplingHigh Energy Physics::ExperimentMatrix element010306 general physicsNuclear theoryPhysical Review D
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On the observability of Majoron emitting double beta decays

1996

Because of the fine--tuning problem in classical Majoron models in recent years several new models were invented. It is pointed out that double beta decays with Majoron emission depend on new matrix elements, which have not been considered in the literature. A calculation of these matrix elements and phase space integrals is presented. We find that for new Majoron models extremely small decay rates are expected.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaNuclear Theory (nucl-th)Matrix (mathematics)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Phase spaceBeta (velocity)ObservabilityMajoron
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Dynamical generation of hyperon resonances

2003

In this talk we report on how, using a chiral unitary approach for the meson--baryon interactions, two octets of $J^{\pi}=1/2^-$ baryon states and a singlet are generated dynamically, resulting in the case of strangeness $S=-1$ in two poles of the scattering matrix close to the nominal $\Lambda(1405)$ resonance. We suggest experiments which could show evidence for the existence of these states.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryScatteringHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyHyperonResonanceFOS: Physical sciencesFísicaStrangenessNuclear physicsBaryonNuclear Theory (nucl-th)Matrix (mathematics)Symmetry breakingSinglet stateNuclear Experiment
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Nucleon strangeness and unitarity

1996

The strange-quark vector current form factors of the nucleon are analyzed within the framework of dispersion relations. Particular attention is paid to contributions made by $K\bar{K}$ intermediate states to the form factor spectral functions. It is shown that, when the $K\bar{K}\to N\bar{N}$ amplitude is evaluated in the Born approximation, the $K\bar{K}$ contributions are identical to those arising from a one-loop calculation and entail a serious violation of unitarity. The mean square strangeness radius and magnetic moment are evaluated by imposing unitarity bounds on the kaon-nucleon partial wave amplitudes. The impact of including the kaon's form factor in the dispersion integrals is a…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryUnitarityNuclear TheoryHigh Energy Physics::PhenomenologyForm factor (quantum field theory)FOS: Physical sciencesStrangenessNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)AmplitudeDispersion relationHigh Energy Physics::ExperimentBorn approximationNuclear ExperimentNucleonS-matrixPhysical Review D
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ISOSPIN MIXING IN THE VICINITY OF THE N = Z LINE

2010

We present the isospin- and angular-momentum-projected nuclear density functional theory (DFT) and its applications to the isospin-breaking corrections to the superallowed beta-decay rates in the vicinity of the N=Z line. A preliminary value obtained for the Cabbibo-Kobayashi-Maskawa matrix element, |V_{ud}|=0.97463(24), agrees well with the recent estimate by Towner and Hardy [Phys. Rev. C{\bf 77}, 025501 (2008)]. We also discuss new opportunities to study the symmetry energy by using the isospin-projected DFT.

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear Theoryta114Nuclear TheoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesGeneral Physics and AstronomyNuclear matterSymmetry (physics)Nuclear Theory (nucl-th)IsospinMatrix elementNuclear Experiment (nucl-ex)Nuclear ExperimentFunctional theoryNuclear ExperimentNuclear densityMixing (physics)Line (formation)International Journal of Modern Physics E
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