Search results for "UNITARITY"

showing 10 items of 245 documents

On the description of non-unitary neutrino mixing

2015

28 pages.- 8 figures.- typos corrected.- modified bounds on non-unitarity parameters.- new figs 3 and 4

PhysicsNuclear and High Energy PhysicsSterile neutrinoParticle physicsUnitarityPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::PhenomenologyPontecorvo–Maki–Nakagawa–Sakata matrixFísicaFOS: Physical sciencesDouble beta decayHigh Energy Physics - ExperimentStandard Model (mathematical formulation)High Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Heavy majorana neutrinosMeasurements of neutrino speedHigh Energy Physics::ExperimentNeutrinoNeutrino oscillation
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Updating the unitarity triangle: top-quark mass versus nonperturbative uncertainties

1994

13 páginas, 3 figuras, 4 tablas.-- arXiv:hep-ph/9407226v1

PhysicsNuclear and High Energy PhysicsTop quarkParticle physicsUnitarityBar (music)High Energy Physics::PhenomenologyHadronFísicaFOS: Physical sciencesHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)High Energy Physics::ExperimentMixing (physics)Physics Letters B
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Non-standard neutrino oscillations: perspective from unitarity triangles

2021

We formulate an alternative approach based on unitarity triangles to describe neutrino oscillations in presence of non-standard interactions (NSI). Using perturbation theory, we derive the expression for the oscillation probability in case of NSI and cast it in terms of the three independent parameters of the leptonic unitarity triangle (LUT). The form invariance of the probability expression (even in presence of new physics scenario as long as the mixing matrix is unitary) facilitates a neat geometric view of neutrino oscillations in terms of LUT. We examine the regime of validity of perturbative expansions in the NSI case and make comparisons with approximate expressions existing in liter…

PhysicsNuclear and High Energy PhysicsUnitarity010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyDegrees of freedom (physics and chemistry)FOS: Physical sciencesQC770-798Invariant (physics)01 natural sciencesHigh Energy Physics - PhenomenologyTheoretical physicsMatrix (mathematics)CP violationHigh Energy Physics - Phenomenology (hep-ph)Nuclear and particle physics. Atomic energy. RadioactivityBeyond Standard Model0103 physical sciencesNeutrino PhysicsPerturbation theory (quantum mechanics)Neutrino010306 general physicsNeutrino oscillationJournal of High Energy Physics
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Pinch technique at two loops: The case of massless Yang-Mills theories

2000

The generalization of the pinch technique beyond one loop is presented. It is shown that the crucial physical principles of gauge-invariance, unitarity, and gauge-fixing-parameter independence single out at two loops exactly the same algorithm which has been used to define the pinch technique at one loop, without any additional assumptions. The two-loop construction of the pinch technique gluon self-energy, and quark-gluon vertex are carried out in detail for the case of mass-less Yang-Mills theories, such as perturbative QCD. We present two different but complementary derivations. First we carry out the construction by directly rearranging two-loop diagrams. The analysis reveals that, quit…

PhysicsNuclear and High Energy PhysicsUnitarityBackground field methodFOS: Physical sciencesFísicaYang–Mills existence and mass gapSymmetry (physics)RenormalizationHigh Energy Physics - PhenomenologyDimensional regularizationsymbols.namesakeTheoretical physicsHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicssymbolsFeynman diagramGauge theoryPhysical Review D
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Role of the f 1 (1285) state in theJ/ψ→ϕK¯K⁎and J / ψ → ϕf 1 (1285) decays

2016

Abstract We study the role of the f 1 ( 1285 ) resonance in the decays of J / ψ → ϕ K ¯ K ⁎ and J / ψ → ϕ f 1 ( 1285 ) . The theoretical approach is based on the results of chiral unitary theory where the f 1 ( 1285 ) resonance is dynamically generated from the K ⁎ K ¯ – c.c. interaction. In order to further test the dynamical nature of the f 1 ( 1285 ) state, we investigate the J / ψ → ϕ K ¯ K ⁎ decay close to the K ¯ K ⁎ threshold and make predictions for the ratio of the invariant mass distributions of the J / ψ → ϕ K ¯ K ⁎ decay and the J / ψ → ϕ f 1 ( 1285 ) partial decay width with all the parameters of the mechanism fixed in previous studies. The results can be tested in future exper…

PhysicsNuclear and High Energy PhysicsUnitarityMeson010308 nuclear & particles physicsState (functional analysis)16. Peace & justice01 natural sciencesOmegaResonance (particle physics)0103 physical sciencesMass spectrumOrder (group theory)Invariant massAtomic physics010306 general physicsMathematical physicsPhysics Letters B
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Low lying S=-1 excited baryons and chiral symmetry

2001

The s-wave meson-baryon interaction in the $S = -1$ sector is studied by means of coupled-channels, using the lowest-order chiral Lagrangian and the N/D method to implement unitarity. The loops are regularized using dimensional renormalization. In addition to the previously studied $\Lambda (1405)$, employing this chiral approach leads to the dynamical generation of two more s-wave hyperon resonances, the $\Lambda(1670)$ and $\Sigma(1620)$ states. We make comparisons with experimental data and look for poles in the complex plane obtaining the couplings of the resonances to the different final states. This allows us to identify the $\Lambda (1405)$ and the $\Lambda(1670)$ resonances with $\b…

PhysicsNuclear and High Energy PhysicsUnitarityNuclear TheoryHigh Energy Physics::PhenomenologyHyperonFísicaSigmaFOS: Physical sciencesLambdaBaryonRenormalizationNuclear Theory (nucl-th)Excited stateComplex planeMathematical physics
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Constraints on the CKM angleγinB0→D¯0K*0andB0→D0K*0from a Dalitz analysis ofD0andD¯0decays toKSπ+π−

2009

We present constraints on the angle γ of the unitarity triangle with a Dalitz analysis of neutral D decays to KSπ+π- from the processes B0→D0K*0 (B0→D0K*0) and B0→D0K*0 (B0→D0K*0) with K*0→K+π- (K*0→K-π+). Using a sample of 371×106 BB pairs collected with the BABAR detector at PEP-II, we constrain the angle γ as a function of rS, the magnitude of the average ratio between b→u and b→c amplitudes. © 2009 The American Physical Society.

PhysicsNuclear physicsNuclear and High Energy PhysicsAmplitudeUnitarity010308 nuclear & particles physicsElectron–positron annihilation0103 physical sciencesDalitz plotFunction (mathematics)010306 general physics01 natural sciencesPhysical Review D
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Determination of γ and−2βsfrom charmless two-body decays of beauty mesons

2015

Using the latest LHCb measurements of time-dependent CP violation in the B-s(0) -> K+K- decay, a U-spin relation between the decay amplitudes of B-s(0) -> K+K- and B-0 -> p(+)p(-) decay processes allows constraints to be placed on the angle gamma of the unitarity triangle and on the B-s(0) mixing phase -2 beta(s). Results from an extended approach, which uses additional inputs on B-0 -> pi(0)pi(0) and B+ -> pi(+)pi(0) decays from other experiments and exploits isospin symmetry, are also presented. The dependence of the results on the maximum allowed amount of U-spin breaking is studied. At 68% probability, the value gamma =( 63.5(-6.7)(+7.2))degrees modulo 180 degrees is determined. In an a…

PhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsAmplitudeMesonUnitarityIsospinPiValue (computer science)CP violationBeta (velocity)Physics Letters B
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Isospin breaking andf0(980)-a0(980)mixing in theη(1405)→π0f0(980)reaction

2012

We make a theoretical study of the eta(1405) -> pi(0)f(0)(980) and eta(1405) -> pi(0)a(0)(980) reactions with an aim to determine the isospin violation and the mixing of the f(0)(980) and a(0)(980) resonances. We make use of the chiral unitary approach where these two resonances appear as composite states of two mesons, dynamically generated by the meson-meson interaction provided by chiral Lagrangians. We obtain a very narrow shape for the f(0)(980) production in agreement with a BES experiment. As to the amount of isospin violation, or f(0)(980) and a(0)(980) mixing, assuming constant vertices for the primary eta(1405) -> pi K-0 (K) over bar and eta(1405) -> pi(0)pi(0)eta production, we f…

PhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMesonUnitarityIsospinPartial wave analysisResonanceHigh Energy Physics::ExperimentAnomaly (physics)Wave functionPhysical Review D
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Hyperon Semileptonic Decays and CKM Unitarity

2005

We perform a new numerical analysis of hyperon semileptonic decays emphasizing the systematic uncertainties. The poor understanding of SU(3) symmetry breaking effects at second order in the vector form factor translates into a large error of |V(us)|. Using our determination |V(us)| = 0.226 +/- 0.005 together with those coming from other sources we test the unitarity of the CKM matrix.

PhysicsNuclear physicsNuclear and High Energy PhysicsParticle physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)UnitarityCabibbo–Kobayashi–Maskawa matrixHyperonForm factor (quantum field theory)FOS: Physical sciencesSymmetry breakingAtomic and Molecular Physics and Optics
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