Search results for "PERTURBATION"

showing 10 items of 811 documents

A measurement of the decay KL→π0γγ

1992

Abstract The full data set of the experiment NA31 at CERN has been used to analyse the decay mode KL→π0γγ. A signal of 63 events has been observed with an estimated background of 6.0±1.7 events, corresponding to a branching ratio of (1.7±0.3)×10−6 consistent with our previous result based on partial statistics. The invariant mass spectrum of the two photons is found to be consistent with chiral perturbation theory, and the decay is dominated by the J = 0 two photon state.

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonChiral perturbation theoryMeson010308 nuclear & particles physicsBranching fractionElementary particle7. Clean energy01 natural sciencesNuclear physicsParticle decay0103 physical sciencesHigh Energy Physics::ExperimentInvariant mass010306 general physicsBosonPhysics Letters B
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Virtual Compton scattering and the generalized polarizabilities of the proton atQ2=0.92and 1.76 GeV2

2012

Virtual Compton Scattering (VCS) on the proton has been studied at Jefferson Lab using the exclusive photon electroproduction reaction (e p --> e p gamma). This paper gives a detailed account of the analysis which has led to the determination of the structure functions P{sub LL}-P{sub TT}/epsilon and P{sub LT}, and the electric and magnetic generalized polarizabilities (GPs) alpha{sub E}(Q{sup 2}) and beta{sub M}(Q{sup 2}) at values of the four-momentum transfer squared Q{sup 2} = 0.92 and 1.76 GeV{sup 2}. These data, together with the results of VCS experiments at lower momenta, help building a coherent picture of the electric and magnetic GPs of the proton over the full measured Q{sup 2}-…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonChiral perturbation theoryProton010308 nuclear & particles physicsStructure functionCompton scattering01 natural sciencesNuclear physicsAmplitudeDispersion relation0103 physical sciencesBeta (velocity)010306 general physicsPhysical Review C
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Matrix elements of decays

2004

We present a numerical computation of matrix elements of ?I = 3/2 K ? ?? decays by using Wilson fermions. In order to extrapolate to the physical point we work at unphysical kinematics and we resort to Chiral Perturbation Theory at the next-to-leading order. In particular we explain the case of the electroweak penguins 07,8 which can contribute significantly in the theoretical prediction of sol|??/?. The study is done at ? = 6.0 on a 243 × 64 lattice.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysical pointChiral perturbation theoryHigh Energy Physics::LatticeLattice (order)Quantum electrodynamicsComputationElectroweak interactionFermionAtomic and Molecular Physics and OpticsNuclear Physics B - Proceedings Supplements
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Radiative and non radiative muon capture on the proton in heavy baryon chiral perturbation theory

1998

We have evaluated the amplitude for muon capture by a proton, mu + p --> n + nu, to O(p^3) within the context of heavy baryon chiral perturbation theory (HBChPT) using the new O(p^3) Lagrangian of Ecker and Mojzis (E&M). We obtain expressions for the standard muon capture form factors and determine three of the coefficients of the E&M Lagrangian, namely, b_7, b_{19}, and b_{23}. We describe progress on the next step, a calculation of the radiative muon capture process, mu + p --> n + nu + gamma.

PhysicsNuclear and High Energy PhysicsParticle physicsProtonHeavy baryon chiral perturbation theoryNuclear TheoryFOS: Physical sciencesContext (language use)Muon captureNuclear Theory (nucl-th)symbols.namesakeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)AmplitudesymbolsRadiative transferLagrangian
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Electromagnetism in nonleptonic weak interactions

2000

16 páginas, 1 figura.-- PACS: 11.30.Rd; 13.25.Es; 13.40.Ks.-- arXiv:hep-ph/0006172v2

PhysicsNuclear and High Energy PhysicsParticle physicsRenormalizationPhotonIsospin violationOrder (ring theory)FOS: Physical sciencesFísicaRenormalizationsymbols.namesakeTheoretical physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)ElectromagnetismEffective lagrangiansChiral perturbation theorysymbolsEffective field theoryNonleptonic weak interactionsLagrangian
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Electromagnetic Corrections for Pions and Kaons : Masses and Polarizabilities

1996

The unknown constants in Chiral Perturbation Theory needed for an all orders analysis of the polarizabilities and electromagnetic corrections to the masses of the pseudo-Goldstone bosons are estimated at leading order in $1/N_c$. We organize the calculation in an $1/N_c$-expansion and separate long- and short-distance physics contributions by introducing an Euclidean cut-off. The long-distance part is evaluated using the ENJL model and the short-distance part using perturbative QCD and factorization. We obtain very good matching between both. We then include these estimates in a full Chiral Perturbation Theory calculation to order $e^2$ $p^2$ for the masses and $p^6$ for the polarizabilitie…

PhysicsNuclear and High Energy PhysicsParticle physicsWork (thermodynamics)Chiral perturbation theoryHigh Energy Physics::PhenomenologyFOS: Physical sciencesOrder (ring theory)Perturbative QCDHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)PionFactorizationEuclidean geometryBoson
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Forward hadron production in pA collisions beyond leading order

2017

In this talk, we report our recent progress on pinning down the cause of negativity in the NLO single inclusive hadron production in pA collisions at forward rapidity.

PhysicsNuclear and High Energy PhysicsParticle physicsta114010308 nuclear & particles physicsHadronperturbative calculationsFOS: Physical sciencesNegativity effect01 natural sciencesNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)color transparencyfactorization0103 physical sciencesProduction (economics)Color transparencyRapidityPerturbation theory (quantum mechanics)010306 general physicsNuclear and Particle Physics Proceedings
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Threshold π0 photoproduction on transverse polarised protons at MAMI

2015

Abstract Polarisation-dependent differential cross sections σ T associated with the target asymmetry T have been measured for the reaction γ p → → p π 0 with transverse target polarisation from π 0 threshold to photon energies of 190 MeV. The data were obtained using a frozen-spin butanol target with the Crystal Ball / TAPS detector set-up and the Glasgow photon tagging system at the Mainz Microtron MAMI. Results for σ T have been used in combination with our previous measurements of the unpolarised cross section σ 0 and the beam asymmetry Σ for a model-independent determination of S- and P-wave multipoles in the π 0 threshold region, which includes for the first time a direct determination…

PhysicsNuclear and High Energy PhysicsPhotonChiral perturbation theoryScatteringmedia_common.quotation_subjectAsymmetryNuclear physicsCross section (physics)Transverse planeAtomic physicsNuclear ExperimentMultipole expansionMicrotronmedia_commonPhysics Letters B
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Threshold electro production of neutral pions at low q2 off the proton and off the deuteron

2000

Abstract The A1 Collaboration performs an extend program to measure threshold production of the neutral pion as test of Heavy Baryon Chiral Perturbation Theory. Starting with direct threshold measurements to extract the s wave amplitudes at threshold we continued with out of plane measurements with polarized beam to access the small p wave amplitudes. Coherent production off the deuteron is the first attempt to access the neutron amplitude in electro production.

PhysicsNuclear and High Energy PhysicsProtonHeavy baryon chiral perturbation theoryNuclear TheoryNuclear physicsPionAmplitudeDeuteriumQuantum electrodynamicsS-waveNeutronNuclear ExperimentBeam (structure)Progress in Particle and Nuclear Physics
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Anomalous chiral perturbation theory meson Lagrangian to orderp6reexamined

2002

We present a revised and extended construction of the mesonic Lagrangian density in chiral perturbation theory (ChPT) at order ${p}^{6}$ in the anomalous (or epsilon) sector, ${\mathcal{L}}_{6,\ensuremath{\epsilon}}.$ After improving several aspects of the strategy we used originally, i.e., a more efficient application of partial integration, the implementation of so-called Bianchi identities, and additional trace relations, we find the new monomial sets to include 24 ${SU(N}_{f}),$ 23 $\mathrm{SU}(3),$ and 5 $\mathrm{SU}(2)$ elements. Furthermore, we introduce 8 supplementary terms due to the extension of the chiral group to ${SU(N}_{f}{)}_{L}\ifmmode\times\else\texttimes\fi{}{SU(N}_{f}{)}…

PhysicsNuclear and High Energy PhysicsRiemann curvature tensorParticle physicsMonomialChiral perturbation theoryTrace (linear algebra)Meson010308 nuclear & particles physicsGroup (mathematics)Order (ring theory)01 natural sciencessymbols.namesake0103 physical sciencessymbols010306 general physicsLagrangianMathematical physicsPhysical Review D
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