Search results for "física nuclear"

showing 10 items of 900 documents

Chiral approach to antikaon s- and p-wave interactions in dense nuclear matter

2006

The properties of the antikaons in nuclear matter are investigated from a chiral unitary approach which incorporates the s- and p-waves of the ${\bar K}N$ interaction. To obtain the in-medium meson-baryon amplitudes we include, in a self-consistent way, Pauli blocking effects, meson self-energies corrected by nuclear short-range correlations and baryon binding potentials. We pay special attention to investigating the validity of the on-shell factorization, showing that it cannot be applied in the evaluation of the in-medium corrections to the p-wave amplitudes. In nuclear matter at saturation energy, the $\Lambda$ and $\Sigma$ develop an attractive potential of about -30 MeV, while the $\Si…

Constitució de la matèriaNuclear TheoryNuclear TheoryFOS: Physical sciencesFísicaNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Collisions (Nuclear physics)Col·lisions (Física nuclear)AntikaonsConstitution of matterNuclear ExperimentPropietats de la matèriaProperties of matter
researchProduct

Present and future bounds on nonstandard neutrino interactions

2003

We consider Non-Standard neutrino Interactions (NSI), described by four-fermion operators of the form ((nu) over bar (alpha)gammanu(beta)) ((f) over bar gammaf), where f is an electron or first generation quark. We assume these operators are generated at dimension greater than or equal to 8, so the related vertices involving charged leptons, obtained by an SU(2) transformation nu(delta)-->e(delta), do not appear at tree level. These related vertices necessarily arise at one loop, via W exchange. We catalogue current constraints from sin(2)theta(W) measurements in neutrino scattering, from atmospheric neutrino observations, from LEP, and from bounds on the related charged lepton operators. W…

CosmologiaPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyHigh Energy Physics::ExperimentPartícules (Física nuclear)
researchProduct

PArthENoPE reloaded

2018

We describe the main features of a new and updated version of the program PArthENoPE, which computes the abundances of light elements produced during Big Bang Nucleosynthesis. As the previous first release in 2008, the new one, PArthENoPE 2.0, will be soon publicly available and distributed from the code site, http://parthenope.na.infn.it. Apart from minor changes, which will be also detailed, the main improvements are as follows. The powerful, but not freely accessible, NAG routines have been substituted by ODEPACK libraries, without any significant loss in precision. Moreover, we have developed a Graphical User Interface (GUI) which allows a friendly use of the code and a simpler implemen…

Cosmology and Nongalactic Astrophysics (astro-ph.CO)FOS: Physical sciencesGeneral Physics and AstronomyAstrophysicscomputer.software_genre01 natural sciencesPartícules (Física nuclear)Physics and Astronomy (all)High Energy Physics - Phenomenology (hep-ph)Big Bang nucleosynthesis0103 physical sciencesCode (cryptography)010306 general physicsGraphical user interfaceParthenopePhysicsCosmologiaPrimordial nucleosynthesi010308 nuclear & particles physicsProgramming languagebusiness.industryCosmologyNeutrino physicHigh Energy Physics - PhenomenologyHardware and ArchitecturebusinesscomputerAstrophysics - Cosmology and Nongalactic Astrophysics
researchProduct

Eta-eta' Photoproduction and the axial isoscalar neutral current coupling

1995

We show that coherentη andη′ photoproduction by means of the Primakoff Effect on the proton depends on the strange component of the neutral axial current coupling. We construct polarization asymmetries that are sensitive to this coupling through theγ−Z interference. Theη′ is not a Goldstone boson of a spontaneously broken chiral symmetry, but a phenomenological analysis of theη andη′ production through chiral perturbation theory allows to calculate the observables of interest. The polarized proton or polarized photon asymmetries are predicted to be close to 10−4 for −q 2∼0.1−0.5 GeV2.

CouplingPhysicsParticle physicsChiral perturbation theoryPhysics and Astronomy (miscellaneous)Neutral currentIsoscalarElementary particlePrime (order theory)Partícules (Física nuclear)Nuclear physicsGoldstone bosonHigh Energy Physics::ExperimentNucleonNuclear ExperimentPrimakoff effectBoson
researchProduct

Enhancement effects in exclusive pi pi production in gamma* gamma scattering

2009

The exclusive pi pi and rho pi production in hard gamma*gamma scattering in the forward kinematical region where the virtual photon is highly off-shell is studied using the gamma -> pi(-) Transition Distribution Amplitudes obtained in realistic models for the pion. For rho pi production we confirm the previous estimates before QCD evolution. Nevertheless. once evolution is taken into account this cross section grows one order of magnitude. In the case of pi pi production we have evaluated the cross section including the pion pole contribution. We observe that this contribution is responsible for an enhancement of two orders of magnitude with respect to the cross section evaluated without th…

Cromodinàmica quànticaPartícules (Física nuclear)
researchProduct

Measurement of dijet production with a veto on additional central jet activity in pp collisions at sqrt(s)=7 TeV using the ATLAS detector

2011

A measurement of jet activity in the rapidity interval bounded by a dijet system is presented. Events are vetoed if a jet with transverse momentum greater than 20 GeV is found between the two boundary jets. The fraction of dijet events that survive the jet veto is presented for boundary jets that are separated by up to six units of rapidity and with mean transverse momentum 50 < p¯T < 500 GeV. The mean multiplicity of jets above the veto scale in the rapidity interval bounded by the dijet system is also presented as an alternative method for quantifying perturbative QCD emission. The data are compared to a next-to-leading order plus parton shower prediction from the powheg-box, an all-order…

DIJETSParticle physicsNuclear and High Energy Physics:Mathematics and natural science: 400::Physics: 430 [VDP]Ciências Naturais::Ciências FísicasAtlas detectorAstrophysics::High Energy Astrophysical Phenomena:Ciências Físicas [Ciências Naturais]Monte Carlo methodFOS: Physical sciencesddc:500.2:Mathematics and natural science: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]01 natural sciences530High Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Rapidityddc:530High Energy PhysicsResummation010306 general physicsParton showerNuclear ExperimentPhysicsScience & TechnologyHadron-Hadron Scattering010308 nuclear & particles physicsSettore FIS/01 - Fisica SperimentaleHigh Energy Physics::PhenomenologyPerturbative QCDATLASBounded functionHADRON-HADRON COLLISIONSTransverse momentumFísica nuclearHigh Energy Physics::ExperimentLHCParticle Physics - Experiment
researchProduct

s-wave charmed baryon resonances from a coupled-channel approach with heavy quark symmetry

2009

We study charmed baryon resonances which are generated dynamically within a unitary meson-baryon coupled channel model that treats the heavy pseudoscalar and vector mesons on equal footing as required by heavy-quark symmetry. It is an extension of recent SU(4) models with t-channel vector meson exchanges to a SU(8) spin-flavor scheme, but differs considerably from the SU(4) approach in how the strong breaking of the flavor symmetry is implemented. Some of our dynamically generated states can be readily assigned to recently observed baryon resonances, while others do not have a straightforward identification and require the compilation of more data as well as an extension of the model to d-w…

DYNAMICSQuarkNuclear and High Energy PhysicsParticle physicsDECAY CONSTANTSField theory (Physics)MesonHigh Energy Physics::LatticeNuclear TheoryFOS: Physical sciencesCHIRAL PERTURBATION-THEORY01 natural sciencesPartícules (Física nuclear)High Energy Physics - Phenomenology (hep-ph)UNITARY APPROACHHadron spectroscopy0103 physical sciencesSCATTERINGSymmetry breakingNuclear Experiment010306 general physicsParticles (Nuclear physics)PhysicsCLEBSCH-GORDAN COEFFICIENTS010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyTeoria de camps (Física)FísicaSymmetry (physics)BaryonPseudoscalarCharmed baryonsHigh Energy Physics - PhenomenologySTATESKAON-NUCLEON INTERACTIONSMESON-MESONHigh Energy Physics::ExperimentBETHE-SALPETER APPROACHPhysical Review D
researchProduct

Study of high-multiplicity three-prong and five-prong τ decays at BABAR

2012

We present measurements of the branching fractions of three-prong and five-prong tau decay modes using a sample of 430 million tau lepton pairs, corresponding to an integrated luminosity of 468 fb(-1), collected with the BABAR detector at the PEP-II asymmetric-energy e_e storage rings at SLAC National Accelerator Laboratory. The tau(-) -> (3 pi)(-) eta nu(tau), tau(-) -> (3 pi)(-) omega nu(tau), and tau(-) f(1) (1285)nu(tau) branching fractions are presented, as well as a new limit on the branching fraction of the second-class current decay tau(-) -> pi(-) eta'(958)nu(tau). We search for the decay mode tau(-) -> K- eta'(958)nu(tau) and for five-prong decay modes with kaons, and place the fi…

Decays of taus; TausNuclear and High Energy PhysicsParticle physicsElectron–positron annihilationDecays of tausPACS: 13.35.Dx 14.60.FgHigh multiplicity01 natural sciencesTausNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Decays of tau010306 general physicsCurrent decayPhysics010308 nuclear & particles physicsBranching fractionLeptons (Física nuclear)Particle physicsHEPLeptons (Nuclear physics)BaBarHigh Energy Physics::ExperimentExperimentsFísica de partículesLepton
researchProduct

Measurement of the inelastic proton-proton cross-section at √s = 7 TeV with the ATLAS detector

2011

The dependence of the rate of proton–proton interactions on the centre-of-mass collision energy, √s, is of fundamental importance for both hadron collider physics and particle astrophysics. The dependence cannot yet be calculated from first principles; therefore, experimental measurements are needed. Here we present the first measurement of the inelastic proton–proton interaction cross-section at a centre-of-mass energy, √s, of 7 TeV using the ATLAS detector at the Large Hadron Collider. Events are selected by requiring hits on scintillation counters mounted in the forward region of the detector. An inelastic cross-section of 60.3±2.1 mb is measured for ξ>5×10[superscript −6], where ξ is ca…

DiffractionAtlas detectorNuclear TheoryGeneral Physics and AstronomyPP01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental TechniquesNuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)ComputingMilieux_MISCELLANEOUSddc:539PhysicsMultidisciplinaryLarge Hadron Colliderphysical sciences; particle physicsSettore FIS/01 - Fisica SperimentaleSoftATLASDiffraction DissociationPhotoproductionElastic-ScatteringScintillation counterComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearLHCddc:500Particle Physics - ExperimentParticle physicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2High-Energies530General Biochemistry Genetics and Molecular BiologyArticleNuclear physicsphysical sciencesinelastic; proton–proton cross-section;ATLAS detector0103 physical sciencesAmplitudesHigh Energy Physicsparticle physics010306 general physicsAstroparticle physicsHardScience & Technology010308 nuclear & particles physicsGeneral ChemistryCollisionExperimental High Energy PhysicsPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentModel
researchProduct

Drift Time Measurement in the ATLAS Liquid Argon Electromagnetic Calorimeter using Cosmic Muons

2010

The ionization signals in the liquid argon of the ATLAS electromagnetic calorimeter are studied in detail using cosmic muons. In particular, the drift time of the ionization electrons is measured and used to assess the intrinsic uniformity of the calorimeter gaps and estimate its impact on the constant term of the energy resolution. The drift times of electrons in the cells of the second layer of the calorimeter are uniform at the level of 1.3% in the barrel and 2.8% in the endcaps. This leads to an estimated contribution to the constant term of (0.29-0.04+0.05)% in the barrel and (0.54-0.04+0.06)% in the endcaps. The same data are used to measure the drift velocity of ionization electrons …

Drift velocityPhysics - Instrumentation and DetectorsPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsInstrumentationFOS: Physical sciencesddc:500.2ElectronAstrophysics::Cosmology and Extragalactic AstrophysicsElectromagnetic CalorimeterATLAS; Drift Time Measurement; Cosmic Muons5307. Clean energy01 natural sciencesPartícules (Física nuclear)High Energy Physics - Experiment010305 fluids & plasmasNuclear physicsHigh Energy Physics - Experiment (hep-ex)Atlas (anatomy)Ionization0103 physical sciencesmedicineFysikddc:530High Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Cosmic MuonsDetectors and Experimental Techniques010306 general physicsEngineering (miscellaneous)Ciencias ExactasDetectors de radiacióPhysicsCalorimeter (particle physics)010308 nuclear & particles physicsAcceleradors de partículesResolution (electron density)Instrumentation and Detectors (physics.ins-det)ATLASliquid argonElectromagnetic calorimetermedicine.anatomical_structureExperimental High Energy PhysicsDrift Time MeasurementPhysical SciencesComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHigh Energy Physics::ExperimentLHC
researchProduct