Search results for "Matrix"

showing 10 items of 3205 documents

Models for neutrino mass with discrete symmetries

2010

Discrete non-abelian flavor symmetries give in a natural way tri-bimaximal (TBM) mixing as showed in a prototype model. However neutrino mass matrix pattern may be very different from the tri-bimaximal one if small deviations of TBM will be observed. We give the result of a model independent analysis for TBM neutrino mass pattern.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsSmall deviationsFOS: Physical sciencesMass matrix01 natural sciencesAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)0103 physical sciencesHomogeneous spaceNeutrino10. No inequality010306 general physicsMixing (physics)Nuclear Physics B - Proceedings Supplements
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Fritzsch neutrino mass matrix fromS3symmetry

2010

We present an extension of the Standard Model (SM) based on the discrete flavor symmetry S3 which gives a neutrino mass matrix with two-zero texture of Fritzsch-type and nearly diagonal charged lepton mass matrix. The model is compatible with the normal hierarchy only and predicts the sine squared of the reactor angle to be 0.01 at the best fit values of solar and atmospheric parameters and maximal leptonic CP violation.

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsTexture (cosmology)High Energy Physics::PhenomenologyDiagonalFOS: Physical sciencesMass matrix01 natural sciencesSymmetry (physics)High Energy Physics - PhenomenologyStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)Physical Sciences0103 physical sciencesCP violationHigh Energy Physics::ExperimentNeutrino010306 general physicsParticle Physics - PhenomenologyLeptonJournal of Physics G: Nuclear and Particle Physics
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Simultaneous measurement of forward-backward asymmetry and top polarization in dilepton final states fromtt¯production at the Tevatron

2015

We present a simultaneous measurement of the forward-backward asymmetry and the top-quark polarization in t (t) over bar production in dilepton final states using 9.7 fb(-1) of proton-antiproton collisions at root s = 1.96 TeV with the D0 detector. To reconstruct the distributions of kinematic observables we employ a matrix element technique that calculates the likelihood of the possible t (t) over bar kinematic configurations. After accounting for the presence of background events and for calibration effects, we obtain a forward-backward asymmetry of A(t (t) over bar) = (15.0 +/- 6.4(stat) +/- 4.9(syst)) % and a top-quark polarization times spin analyzing power in the beam basis of kappa P…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsmedia_common.quotation_subjectTevatronObservableForward backwardPolarization (waves)01 natural sciencesAsymmetryNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentMatrix elementNuclear Experiment010306 general physicsLeptonmedia_commonPhysical Review D
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Probing CPT in transitions with entangled neutral kaons

2015

In this paper we present a novel CPT symmetry test in the neutral kaon system based, for the first time, on the direct comparison of the probabilities of a transition and its CPT reverse. The required interchange of in ↔ out states for a given process is obtained exploiting the Einstein-Podolsky-Rosen correlations of neutral kaon pairs produced at a ϕ-factory. The observable quantities have been constructed by selecting the two semileptonic decays for flavour tag, the ππ and 3π 0 decays for CP tag and the time orderings of the decay pairs. The interpretation in terms of the standard Weisskopf-Wigner approach to this system, directly connects CPT violation in these observables to the violati…

PhysicsNuclear and High Energy PhysicsParticle physicsCPT symmetryHigh Energy Physics::PhenomenologyFOS: Physical sciencesFísicaObservableQuantum entanglementDiscrete and finite symmetries; Kaon Physics; CP violationMass matrixHigh Energy Physics - PhenomenologyKaon Physicssymbols.namesakeHigh Energy Physics - Phenomenology (hep-ph)CP violationsymbolsCP violationDiscrete and finite symmetriesHigh Energy Physics::ExperimentEPR paradoxSensitivity (control systems)Spurious relationshipJournal of High Energy Physics
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CKM matrix and fermion masses in the dualized standard model

1997

A Dualized Standard Model recently proposed affords a natural explanation for the existence of Higgs fields and of exactly 3 generations of fermions, while giving at the same time the observed fermion mass hierarchy together with a tree-level CKM matrix equal to the identity matrix. It further suggests a method for generating from loop corrections the lower generation masses and nondiagonal CKM matrix elements. In this paper, the proposed calculation is carried out to 1-loop. It is found first that with the method suggested one can account readily for the masses of the second generation fermions as a `leakage' from the highest generation. Then, with the Yukawa couplings fixed by fitting the…

PhysicsNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixElectroweak interactionHigh Energy Physics::PhenomenologyIdentity matrixYukawa potentialFOS: Physical sciencesFísicaFermionHigh Energy Physics - PhenomenologyStandard Model (mathematical formulation)High Energy Physics - Phenomenology (hep-ph)Higgs bosonFree parameter
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New Physics and Evidence for a Complex CKM

2005

We carefully analyse the present experimental evidence for a complex CKM matrix, even allowing for New Physics contributions to $\epsilon_{K}$, $a_{J/\Psi K_S}$, $\Delta M_{B_{d}}$, $\Delta M_{B_{s}}$, and the $\Delta I=1/2$ piece of $B\to\rho\rho$ and $B\to\rho\pi$. We emphasize the crucial r\^ ole played by the angle $\gamma$ in both providing irrefutable evidence for a complex CKM matrix and placing constraints on the size of NP contributions. It is shown that even if one allows for New Physics a real CKM matrix is excluded at a 99.92% C.L., and the probability for the phase $\gamma$ to be in the interval $[-170^\circ;-10^\circ]\cup [10^\circ;170^\circ]$ is 99.7%.

PhysicsNuclear and High Energy PhysicsParticle physicsCabibbo–Kobayashi–Maskawa matrixPhysics beyond the Standard ModelPhase (waves)FOS: Physical sciencesFísicaHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Interval (graph theory)High Energy Physics::ExperimentParticle Physics - Phenomenology
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Chiral fermions and gauge fixing in five-dimensional theories

2001

We study in detail the issue of gauge-fixing in theories with one universal extra dimension, i.e. theories where both bosons and fermions display Kaluza-Klein (KK) excitations. The extra dimension is compactified using the standard orbifold construction for a massless chiral fermion. We carry out the gauge-fixing procedure at the level of the five-dimensional theory and determine the tree-level propagators and interaction vertices needed for performing perturbative calculations with the effective four-dimensional theory resulting after the compactification. The gauge-independence of the tree-level S-matrix involving massive KK modes is verified using specific examples. In order to obtain ma…

PhysicsNuclear and High Energy PhysicsParticle physicsCompactification (physics)High Energy Physics::LatticeFOS: Physical sciencesPropagatorFísicaFermionUniversal extra dimensionHigh Energy Physics - PhenomenologyTheoretical physicsHigh Energy Physics::TheoryHigh Energy Physics - Phenomenology (hep-ph)Gauge anomalyOrbifoldGauge fixingS-matrix
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Three-body resonances in two-meson-one-baryon systems

2007

We report four $\Sigma$'s and three $\Lambda$'s, in the 1500 - 1800 MeV region, as two meson - one baryon S-wave $(1/2)^+$ resonances. We solve Faddeev equations in the coupled channel approach. The invariant mass of one of the meson-baryon pairs and that of the three particles have been varied and peaks in the squared three body $T$-matrix have been found very close to the existing $S$ = -1, $J^P= 1/2^+$ low lying baryon resonances. The input two-body $t$-matrices for meson-meson and meson-baryon interaction have been calculated by solving the Bethe-Salpeter equation with the potentials obtained in the chiral unitary approach.

PhysicsNuclear and High Energy PhysicsParticle physicsFaddeev equationsBethe–Salpeter equationMesonNuclear TheoryHigh Energy Physics::LatticeHigh Energy Physics::PhenomenologyNuclear TheoryFOS: Physical sciencesFísicaFew-body systemsThree-body problemBaryonNuclear Theory (nucl-th)Invariant massHigh Energy Physics::ExperimentNuclear ExperimentS-matrix
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Lepton Transmutation in the Dualized Standard Model

2002

The successful explanation of fermion mixing and of the fermion mass hierarchy by the Dualized Standard Model (DSM) scheme is based on the premises of a fermion mass matrix rotating in generation space with changing scales at a certain speed, which could in principle lead to sizeable flavour-violation observable in high sensitivity experiments such as BaBar. However, a full perturbative calculation to 1-loop order reported here shows that this kinematical, flavour-violating effect of a rotating mass matrix is off-set in the DSM by parallel effects from rotating wave functions and vertices giving in the end only very small flavour-violations which are unlikely to be detectable by present exp…

PhysicsNuclear and High Energy PhysicsParticle physicsFísicaFOS: Physical sciencesObservableFermionSpace (mathematics)Mass matrixMatrix (mathematics)Standard Model (mathematical formulation)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Mixing (physics)Lepton
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SU(4) breaking, allowed transitions and total muon capture rates in nuclei

1973

The authors study muon capture rates in light nuclei and show that one can evaluate them in a model-independent way by correcting the Primakoff closure approximation to the first order in the neutrino energy dependence. In this framework the interplay between the existence of allowed transitions and SU(4) breaking is analyzed. In the correction to the first order in the neutrino energy dependence by a sum rule, Majorana and SU(4) breaking potentials are taken into account. The method is also applied to single multipolar transitions, in particular for the dipole transitions. General considerations are illustrated for /sup 6/Li and /sup 12/C by explicit calculations. The stability of the resu…

PhysicsNuclear and High Energy PhysicsParticle physicsFísicaMuon captureNuclear physicsMAJORANADipoleMatrix (mathematics)Symmetry breakingSum rule in quantum mechanicsNeutrinoMixing (physics)Nuclear Physics
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