Search results for "PERTURBATION"

showing 10 items of 811 documents

The width of the omega meson in the nuclear medium

2013

We evaluate the width of the omega meson in nuclear matter. We consider the free decay mode of the omega into three pions, which is dominated by rho IEuro decay, and replace the rho and pi propagators by their medium-modified ones. We also take into account the quasielastic and inelastic processes induced by a vector-baryon interaction dominated by vector meson exchange, as well as the contributions coming from the mechanism with medium-modified K , propagators. We obtain a substantial increase of the omega width in the medium, reaching a value of 121 +/- 10 MeV at normal nuclear matter density for an omega at rest, which comes mainly from omega N -> pi pi N, omega NN -> pi NN processes ass…

Nuclear and High Energy PhysicsParticle physicsMesonNuclear TheoryNuclear TheoryNuclear physicsFOS: Physical sciences7. Clean energy01 natural sciencesOmegaMomentumNuclear Theory (nucl-th)PionChiral perturbation theory0103 physical sciencesMesons (Nuclear physics)Vector mesonMesons (Física nuclear)Nuclear structure010306 general physicsNuclear ExperimentPhysicsEstructura nuclear010308 nuclear & particles physicsPropagatorHeavy-Ion CollisionsFísicaNuclear matterFísica nuclearHigh Energy Physics::ExperimentHidden Local SymmetryBar (unit)
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Running of the Charm-Quark Mass from HERA Deep-Inelastic Scattering Data

2017

Physics letters / B 775, 233 - 238 (2017). doi:10.1016/j.physletb.2017.11.002

Nuclear and High Energy PhysicsParticle physicsPhotonHigh Energy Physics::LatticeFOS: Physical sciencesContext (language use)53001 natural sciencesCharm quarkrenormalizationNuclear physicsHigh Energy Physics - Phenomenology (hep-ph)deep inelastic scattering0103 physical sciencesddc:530Charm (quantum number)quantum chromodynamics: perturbation theory010306 general physicsPhysicsQuantum chromodynamics010308 nuclear & particles physicsScatteringPhysicsHigh Energy Physics::Phenomenologyhigher-order: 1charm: productionHERADeep inelastic scatteringlcsh:QC1-999quark: massHigh Energy Physics - PhenomenologyDESY HERA Storscale dependence[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]High Energy Physics::Experiment[ PHYS.HPHE ] Physics [physics]/High Energy Physics - Phenomenology [hep-ph]charmlcsh:Physics
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The radiative decay of the Lambda(1405) and its two-pole structure

2007

We evaluate theoretically the radiative decay widths into $\gamma\Lambda$ and $\gamma\Sigma^0$ of the two poles of the $\Lambda(1405)$ found in chiral unitary theories and we find quite different results for each of the two poles. We show that, depending on which reaction is used to measure the $\Lambda(1405)$ radiative decays, one gives more weight to one or the other pole, resulting in quite different shapes in the $\gamma\Lambda(\Sigma^0)$ invariant mass distributions. Our results for the high-energy pole agree with those of the empirical determination of the $\gamma\Lambda$ and $\gamma\Sigma^0$ radiative widths (based on an isobar model fitting of the $K^-p$ atom data), which are someti…

Nuclear and High Energy PhysicsParticle physicsRadiative decayStructure (category theory)radiative decay [Lambda(1405)]chiral [perturbation theory]Lambda(Sigma0 photon) [mass spectrum]Measure (mathematics)Lambda(1405) --> Lambda photonK- p --> Lambda pi0 photonK- p --> Sigma0 pi0 photonAtompi- p --> Lambda K0 photonpi- p --> Sigma0 K0 photonRadiative transferddc:530Invariant massnumerical calculationsPhysicsLambda(1405) --> Sigma0 photonSigma0inelastic scattering [K- p]Físicapole [approximation]hadroproduction [Lambda(1405)]High Energy Physics - Phenomenology(Lambda photon) [mass spectrum]Isobarinelastic scattering [pi- p]hadroproduction [hyperon]width [Lambda(1405)]
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Precision measurement of the ratio of the charged kaon leptonic decay rates

2013

A precision measurement of the ratio RK of the rates of kaon leptonic decays K+- --> e nu and K+- --> mu nu with the full data sample collected by the NA62 experiment at CERN in 2007-2008 is reported. The result, obtained by analysing ~150000 reconstructed K+- --> e nu candidates with 11% background contamination, is RK = (2.488+-0.010)*10^{-5}, in agreement with the Standard Model expectation.

Nuclear and High Energy PhysicsParticle physicsstandard modelFOS: Physical sciencesNA62 experiment01 natural sciencesHigh Energy Physics - ExperimentStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)lepton universalityRare kaon decays; chiral perturbation theoryLepton universality; Charged Kaon Decay0103 physical scienceskaon decays leptonic decays lepton universality010306 general physicschiral perturbation theoryPhysicsleptonic decaysLarge Hadron Colliderkaon decays010308 nuclear & particles physicscharged kaon3. Good healthCharged Kaon DecayRare kaon decaysKaon rare decaysFull dataKaon rare decays; branching ratio; charged kaon; leptonic decays; standard modelbranching ratioParticle Physics - ExperimentLepton universality
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Compton scattering off pions and electromagnetic polarizabilities

2019

The electric ($\alpha_\pi$) and magnetic ($\beta_\pi$) Compton polarizabilities of both the charged and the neutral pion are of fundamental interest in the low-energy sector of quantum chromodynamics (QCD). Pion polarizabilities affect the shape of the $\gamma\pi\to\gamma\pi$ Compton scattering angular distribution at back scattering angles and $\gamma\gamma\to\pi\pi$ absolute cross sections. Theory derivations are given of the $\gamma\pi\to\gamma\pi$ Compton scattering differential cross section, dispersion relations, and sum rules in terms of the polarizabilities. We review experimental charged and neutral polarizability studies and theoretical predictions. The $\pi^0$ polarizabilities we…

Nuclear and High Energy PhysicsPhotonChiral perturbation theoryNuclear TheoryAstrophysics::High Energy Astrophysical PhenomenaHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesVirtual particle01 natural sciencesHigh Energy Physics - ExperimentNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Pion0103 physical sciencesNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear ExperimentQuantum chromodynamicsPhysics010308 nuclear & particles physicsCompton scatteringAstronomy and AstrophysicsAtomic and Molecular Physics and OpticsHigh Energy Physics - PhenomenologyHigh Energy Physics::ExperimentSum rule in quantum mechanicsCrystal BallInternational Journal of Modern Physics A
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$W^{+}W^{-}$ production at the LHC: fiducial cross sections and distributions in NNLO QCD

2016

We consider QCD radiative corrections to $W^+W^-$ production at the LHC and present the first fully differential predictions for this process at next-to-next-to-leading order (NNLO) in perturbation theory. Our computation consistently includes the leptonic decays of the $W$ bosons, taking into account spin correlations, off-shell effects and non-resonant contributions. Detailed predictions are presented for the different-flavour channel $pp\to\mu^+e^-\nu_\mu {\bar \nu}_e+X$ at $\sqrt{s}=8$ and $13$ TeV. In particular, we discuss fiducial cross sections and distributions in the presence of standard selection cuts used in experimental $W^+W^-$ and $H\to W^+W^-$ analyses at the LHC. The inclus…

Nuclear and High Energy Physicsleptonic decay010308 nuclear & particles physics530 Physicsoff-shell [effect]High Energy Physics::LatticeHigh Energy Physics::PhenomenologyFOS: Physical sciences10192 Physics Institute01 natural sciences2 [higher-order]High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)CERN LHC Collcorrelation [spin]radiative correction [quantum chromodynamics]0103 physical sciencesddc:530High Energy Physics::Experimentexpansion 1/N3106 Nuclear and High Energy Physics010306 general physicsperturbation theoryJHEP
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Experiments at the electron accelerator MAMI

2008

Nuclear physicsPhysicsChiral perturbation theorylawElectric form factorParticle acceleratorlaw.invention
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Measurement of ππ Scattering Lengths from and Decays

2011

In the last few years it has become possible to study low energy ππ scattering with high precision in kaon decays, thanks to the high statistics measurements of K ± → π ± π 0 π 0 ( K 3 π ) and K ± → π + π − e ± ν ( K e 4 ) decays performed by the NA48/2 experiment at the CERN SPS. In K ± → π ± π 0 π 0 , at the π + π − threshold, the π 0 π 0 mass spectrum exhibits a Wigner-cusp, from which the scattering lengths a 0 and a 2 are extracted. From the study of K e 4 decays a similar precision, but quite independent measurement of a 0 and a 2 can be obtained. The combination of both measurements provides one of the most stringent tests of Chiral Perturbation Theory.

Nuclear physicsPhysicsNuclear and High Energy PhysicsLow energyLarge Hadron ColliderChiral perturbation theoryScatteringMass spectrumAtomic and Molecular Physics and OpticsNuclear Physics B - Proceedings Supplements
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The longitudinal muon polarization in KL → μ+μ-

1991

17 páginas, 3 figuras, 1 tabla.-- CERN-TH-6035-91 ; UWTHPH-1991-9.

Nuclear physicsPhysicsNuclear and High Energy PhysicsMuonChiral perturbation theoryAstrophysics::High Energy Astrophysical PhenomenaAnalytical chemistryFísicaPolarization (waves)Particle Physics - Phenomenology
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A new measurement of the K±→π±γγ decay at the NA48/2 experiment

2014

Abstract The NA48/2 experiment at CERN collected two data samples with minimum bias trigger conditions in 2003 and 2004. A measurement of the rate and dynamic properties of the rare decay K ± → π ± γ γ from these data sets based on 149 decay candidates with an estimated background of 15.5 ± 0.7 events is reported. The model-independent branching ratio in the kinematic range z = ( m γ γ / m K ) 2 > 0.2 is measured to be B MI ( z > 0.2 ) = ( 0.877 ± 0.089 ) × 10 − 6 , and the branching ratio in the full kinematic range assuming a particular Chiral Perturbation Theory description to be B ( K π γ γ ) = ( 0.910 ± 0.075 ) × 10 − 6 .

Nuclear physicsPhysicsNuclear and High Energy PhysicsParticle decayPionChiral perturbation theoryMesonBranching fractionHadronAnalytical chemistryRadioactive decayDimensionless quantityPhysics Letters B
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