Search results for "Pion"

showing 10 items of 1304 documents

Observation of the decayB¯0→Λc+p¯π0

2010

In a sample of 467 x 10(6) B (B) over bar pairs collected with the BABAR detector at the PEP- II collider at SLAC we have observed the decay (B) over bar (0) -> Lambda(+)(c)(p) over bar pi(0) and measured the branching fraction to be (1.94 +/- 0.17 +/- 0.14 +/- 0.50 x 10(-4), where the uncertainties are statistical, systematic, and the uncertainty on the Lambda(+)(c) -> pK(-)pi(+) branching fraction, respectively. We determine an upper limit of 1.5 x 10(-6) at 90% C.L. for the product branching fraction B((B) over bar (0) -> Sigma(+)(c) (2455)(p) over bar) x B(Lambda(+)(c) -> pK(-) pi(+)). Furthermore, we observe an enhancement at the threshold of the invariant mass of the baryon- antibaryo…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsBranching fractionElectron–positron annihilationAnalytical chemistryLambda01 natural sciencesCharmed baryonsParticle decayPion0103 physical sciencesB mesonAtomic physics010306 general physicsBar (unit)Physical Review D
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Magnetic field driven enhancement of the weak decay width of charged pions

2020

We study the effect of a uniform magnetic field B→ on the decays π⁻ → l⁻ ν⁻l, where l⁻ = e⁻, μ⁻, carrying out a general analysis that includes four π⁻ decay constants. Taking the values of these constants from a chiral effective Nambu-Jona-Lasinio (NJL) model, it is seen that the total decay rate gets strongly increased with respect to the B = 0 case, with an enhancement factor ranging from ∼ 10 for eB = 0.1 GeV² up to ∼ 10³ for eB = 1 GeV². The ratio between electronic and muonic decays gets also enhanced, reaching a value of about 1 : 2 for eB = 1 GeV². In addition, we find that for large B the angular distribution of outgoing antineutrinos shows a significant suppression in the direction…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsHigh Energy Physics - Lattice (hep-lat)FísicaFOS: Physical sciences//purl.org/becyt/ford/1.3 [https]QCD Phenomenology7. Clean energy01 natural sciencesMagnetic fieldNuclear physics//purl.org/becyt/ford/1 [https]High Energy Physics - PhenomenologyPionHigh Energy Physics - LatticeHigh Energy Physics - Phenomenology (hep-ph)0103 physical scienceslcsh:QC770-798lcsh:Nuclear and particle physics. Atomic energy. RadioactivityHigh Energy Physics::Experiment010306 general physicsCiencias Exactas
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Production of excited double hypernuclei via Fermi breakup of excited strange systems

2011

Precise spectroscopy of multi-strange hypernuclei provides a unique chance to explore the hyperon-hyperon interaction. In the present work we explore the production of excited states in double hypernuclei following the micro-canonical break-up of an initially excited double hypernucleus which is created by the absorption and conversion of a stopped $\Xi^{-}$ hyperon. Rather independent on the spectrum of possible excited states in the produced double hypernuclei the formation of excited states dominates in our model. For different initial target nuclei which absorb the $\Xi^-$, different double hypernuclei nuclei dominate. Thus the ability to assign the various observable $\gamma$-transitio…

PhysicsNuclear and High Energy Physics010308 nuclear & particles physicsNuclear TheoryHyperonFOS: Physical sciencesObservableHypernucleus01 natural sciencesSpectral lineNuclear physicsPionExcited state0103 physical sciencesNuclear Experiment (nucl-ex)Atomic physics010306 general physicsSpectroscopyNuclear ExperimentNuclear ExperimentFermi Gamma-ray Space Telescope
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The asymmetry in π−3He scattering

1992

Abstract We show that the π + − 3 He asymmetry data obtained in a recent TRIUMF experiment at T π = 100 MeV can be understood in terms of the elementary π N amplitudes. Through a comparison to a full optical-potential calculation that employs realistic Faddeev wave functions for the trinucleon we show that all nuclear-structure dependence cancels for A y at lower energies. At higher pion energies around the Δ-resonance region the sign flip of A y offers the possibility of extracting information about the smaller partial waves.

PhysicsNuclear and High Energy PhysicsAmplitudePionScatteringQuantum electrodynamicsmedia_common.quotation_subjectNuclear TheoryNuclear ExperimentWave functionAsymmetrySign (mathematics)media_commonNuclear Physics A
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First observation and measurement of the decay K±→π±e+e−γ

2008

Abstract Using the full data set of the NA48/2 experiment, the decay K ± → π ± e + e − γ is observed for the first time, selecting 120 candidates with 7.3 ± 1.7 estimated background events. With K ± → π ± π D 0 as normalisation channel, the branching ratio is determined in a model-independent way to be Br ( K ± → π ± e + e − γ , m e e γ > 260  MeV / c 2 ) = ( 1.19 ± 0.12 stat ± 0.04 syst ) × 10 −8 . This measured value and the spectrum of the e + e − γ invariant mass allow a comparison with predictions of chiral perturbation theory.

PhysicsNuclear and High Energy PhysicsAntiparticleChiral perturbation theoryMeson010308 nuclear & particles physicsBranching fractionHadronAnalytical chemistry01 natural sciencesNuclear physicsParticle decayPion0103 physical sciences010306 general physicsDimensionless quantityPhysics Letters B
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Search forCPviolation in the decayD±→KS0π±

2011

We report on a search for CP violation in the decay D{sup {+-}} {yields} K{sub S}{sup 0}{pi}{sup {+-}} using a data set corresponding to an integrated luminosity of 469 fb{sup -1} collected with the BABAR detector at the PEP-II asymmetric energy e{sup +}e{sup -} storage rings. The CP-violating decay rate asymmetry A{sub CP} is determined to be (-0.44 {+-} 0.13(stat) {+-} 0.10(syst))%, consistent with zero at 2.7 {sigma} and with the standard model prediction of (-0.332 {+-} 0.006)%. This is currently the most precise measurement of this parameter.

PhysicsNuclear and High Energy PhysicsAntiparticleParticle physicsMeson010308 nuclear & particles physicsHadron01 natural sciencesNuclear physicsParticle decayPion0103 physical sciencesCP violation010306 general physicsEnergy (signal processing)LeptonPhysical Review D
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On the quasi-elastic neutrino reaction in deuterium in the forward direction

1972

Forward cross-section of the reaction nu +d to mu /sup -/+p+p is studied under different assumptions. It is shown that a value E/sup -2 / (d sigma /d Omega ) approximately=0.27*10/sup -38/ cm/sup 2//sr GeV /sup 2/ is expected independent of the incident neutrino spectrum shape. Relativistic effects and one-pion exchange contributions have been estimated. (10 refs).

PhysicsNuclear and High Energy PhysicsAstrophysics::High Energy Astrophysical PhenomenaFísicaNuclear physicsTheory of relativityPionDeuteriumHigh Energy Physics::ExperimentAtomic physicsNeutrinoNuclear ExperimentRelativistic quantum chemistryParticle Physics - PhenomenologyPhysics Letters B
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Correlators of left charges and weak operators in finite volume chiral perturbation theory

2002

We compute the two-point correlator between left-handed flavour charges, and the three-point correlator between two left-handed charges and one strangeness violating \Delta I=3/2 weak operator, at next-to-leading order in finite volume SU(3)_L x SU(3)_R chiral perturbation theory, in the so-called epsilon-regime. Matching these results with the corresponding lattice measurements would in principle allow to extract the pion decay constant F, and the effective chiral theory parameter g_27, which determines the \Delta I = 3/2 amplitude of the weak decays K to \pi\pi as well as the kaon mixing parameter B_K in the chiral limit. We repeat the calculations in the replica formulation of quenched c…

PhysicsNuclear and High Energy PhysicsChiral perturbation theoryFinite volume methodHigh Energy Physics::LatticeFlavourHigh Energy Physics - Lattice (hep-lat)FOS: Physical sciencesFísicaParticle Physics - LatticeStrangenessweak decaysOperator (computer programming)AmplitudeHigh Energy Physics - Latticechiral Lagrangianslattice QCDLattice (order)kaon physicsPion decay constantMathematical physics
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Recent developments in effective field theory

2007

We will give a short introduction to the one-nucleon sector of chiral perturbation theory and will address the issue of a consistent power counting and renormalization. We will discuss the infrared regularization and the extended on-mass-shell scheme. Both allow for the inclusion of further degrees of freedom beyond pions and nucleons and the application to higher-loop calculations. As applications we consider the chiral expansion of the nucleon mass to order O(q^6) and the inclusion of vector and axial-vector mesons in the calculation of nucleon form factors.

PhysicsNuclear and High Energy PhysicsChiral perturbation theoryMesonNuclear TheoryHigh Energy Physics::LatticeNuclear TheoryDegrees of freedom (statistics)FOS: Physical sciencesRenormalizationNuclear Theory (nucl-th)Theoretical physicsPionRegularization (physics)Effective field theoryNucleonNuclear Experiment
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Generalized polarizabilities of the pion in chiral perturbation theory

1999

We present a calculation of the virtual Compton scattering amplitude for $\gamma^\ast+\pi\to \gamma+\pi$ in the framework of chiral perturbation theory at ${\cal O}(p^4)$. We explicitly derive expressions for generalized electromagnetic polarizabilities and discuss alternative definitions of these quantities.

PhysicsNuclear and High Energy PhysicsChiral perturbation theoryNuclear TheoryAstrophysics::High Energy Astrophysical PhenomenaCompton scatteringFOS: Physical sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)High Energy Physics - Experiment (hep-ex)High Energy Physics - PhenomenologyAmplitudePionHigh Energy Physics - Phenomenology (hep-ph)Quantum mechanicsQuantum electrodynamicsNuclear Experiment (nucl-ex)Nuclear theoryNuclear Experiment
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