Search results for "Proton"

showing 10 items of 5886 documents

Midrapidity Antiproton-to-Proton Ratio inppCollisons ats=0.9and 7 TeV Measured by the ALICE Experiment

2010

The ratio of the yields of antiprotons to protons in pp collisions has been measured by the ALICE experiment at root s = 0.9 and 7 TeV during the initial running periods of the Large Hadron Collider. The measurement covers the transverse momentum interval 0.45 < p(t) < 1.05 GeV/c and rapidity vertical bar y vertical bar < 0.5. The ratio is measured to be R-vertical bar y vertical bar<0.5 = 0.957 +/- 0.006(stat) +/- 0.0014(syst) at 0.9 Tev and R-vertical bar y vertical bar<0.5 = 0.991 +/- 0.005 +/- 0.014(syst) at 7 TeV and it is independent of both rapidity and transverse momentum. The results are consistent with the conventional model of baryon-number transport and set stringent limits on a…

PhysicsParticle physicsLarge Hadron ColliderProton010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyHadronGeneral Physics and Astronomy01 natural sciences7. Clean energyParticle identificationBaryonNuclear physicsAntiproton0103 physical sciencesHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsBar (unit)Physical Review Letters
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Dielectron production in Au + Au collisions atsNN=200GeV

2016

We present measurements of e+e- production at midrapidity in Au+Au collisions at sNN=200 GeV. The invariant yield is studied within the PHENIX detector acceptance over a wide range of mass (mee<5 GeV/c2) and pair transverse momentum (pT<5 GeV/c) for minimum bias and for five centrality classes. The e+e- yield is compared to the expectations from known sources. In the low-mass region (mee=0.30-0.76 GeV/c2) there is an enhancement that increases with centrality and is distributed over the entire pair pT range measured. It is significantly smaller than previously reported by the PHENIX experiment and amounts to 2.3±0.4(stat)±0.4(syst)±0.2(model) or to 1.7±0.3(stat)±0.3(syst)±0.2(model) for min…

PhysicsParticle physicsMeson010308 nuclear & particles physicsDalitz plot01 natural sciencesSuper Proton SynchrotronParticle identificationNuclear physicsPair production0103 physical sciencesHigh Energy Physics::ExperimentRapidityPHENIX detectorNuclear Experiment010306 general physicsGlauberPhysical Review C
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Search for a Light Higgs Boson Decaying to Long-Lived Weakly Interacting Particles in Proton-Proton Collisions ats=7  TeVwith the ATLAS Detector

2012

A search for the decay of a light Higgs boson (120-140 GeV) to a pair of weakly interacting, long-lived particles in 1.94 fb(-1) of proton-proton collisions at root s = 7 TeV recorded in 2011 by the ATLAS detector is presented. The search strategy requires that both long-lived particles decay inside the muon spectrometer. No excess of events is observed above the expected background and limits on the Higgs boson production times branching ratio to weakly interacting, long-lived particles are derived as a function of the particle proper decay length.

PhysicsParticle physicsMesonProton010308 nuclear & particles physicsBranching fractionHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyParticle acceleratorSupersymmetry01 natural scienceslaw.inventionMassless particleNuclear physicsParticle decaylaw0103 physical sciencesHiggs bosonHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review Letters
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Photoproduction ofπ0Mesons off Neutrons in the Nucleon Resonance Region

2014

Precise angular distributions have been measured for the first time for the photoproduction of π0 mesons off neutrons bound in the deuteron. The effects from nuclear Fermi motion have been eliminated by a complete kinematic reconstruction of the final state. The influence of final-state-interaction effects has been estimated by a comparison of the reaction cross section for quasifree protons bound in the deuteron to the results for free protons and then applied as a correction to the quasifree neutron data. The experiment was performed at the tagged photon facility of the Mainz Microtron MAMI with the Crystal Ball and TAPS detector setup for incident photon energies between 0.45 and 1.4 GeV…

PhysicsParticle physicsMesonProtonNuclear TheoryGeneral Physics and AstronomyPhoton energy7. Clean energyNuclear physicsIsospinNeutronNuclear ExperimentNucleonMicrotronCrystal BallPhysical Review Letters
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Neutrinos from the primary proton–proton fusion process in the Sun

2014

International audience; In the core of the Sun, energy is released through sequences of nuclear reactions that convert hydrogen into helium. The primary reaction is thought to be the fusion of two protons with the emission of a low-energy neutrino. These so-called pp neutrinos constitute nearly the entirety of the solar neutrino flux, vastly outnumbering those emitted in the reactions that follow. Although solar neutrinos from secondary processes have been observed, proving the nuclear origin of the Sun's energy and contributing to the discovery of neutrino oscillations, those from proton-proton fusion have hitherto eluded direct detection. Here we report spectral observations of pp neutrin…

PhysicsParticle physicsMultidisciplinaryProtonSolar neutrinoAstrophysics::High Energy Astrophysical PhenomenaNuclear TheorySolar neutrino problemNuclear physicsNeutrino detectorPhysics::Space PhysicsAstrophysics::Solar and Stellar AstrophysicsMeasurements of neutrino speedAstrophysics::Earth and Planetary AstrophysicsNeutrino astronomyNeutrino[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph]Nuclear ExperimentBorexino
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The GDH experiment at MAMI

1999

Abstract The Gerasimov-Drell-Hearn (GDH) sum rule connects the helicity dependent photoabsorption cross section with the anomalous magnetic moment of the nucleon. The GDH-collaboration is measuring the total cross section of circularly polarized photons with longitudinally polarized protons to check this sum rule experimentally to do a further progress in the investigation of the spin structure of the nucleon. The experiment has been started using the polarized electron beam of the Mainz electron accelerator MAMI in the energy range 200 – 800 MeV and will be continued at the Bonn accelerator ELSA up to an energy of about 3 GeV. We have finished the datav taking period at MAMI for the proton…

PhysicsParticle physicsNuclear and High Energy PhysicsPhotonProtonAnomalous magnetic dipole momentNuclear TheoryParticle acceleratorHelicityAtomic and Molecular Physics and Opticslaw.inventionNuclear physicslawPhysics::Accelerator PhysicsSum rule in quantum mechanicsNuclear ExperimentNucleonSpin-½Nuclear Physics A
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Pion Photo- and Electroproduction on the Proton

1999

Using a unitary isobar model a new operator for pion photo- and electroproduction has been developed for nuclear applications at photon equivalent energies up to 1 GeV. The model contains Born terms, vector mesons and nucleon resonances (P 33(1232), P 11(1440), D 13(1520), S 11(1535), F 15(1680), and D 33(1700)). Within this model we have obtained good agreement with the experimental data for pion photo- and electroproduction on the nucleon for both differential cross sections and polarization observables.

PhysicsParticle physicsPhotonPionMesonProtonOperator (physics)Nuclear TheoryPolarization observablesIsobarHigh Energy Physics::ExperimentNuclear ExperimentNucleon
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Measurement of the transverse target and beam-target asymmetries in η meson photoproduction at MAMI

2014

We present new data for the transverse target asymmetry T and the very first data for the beam-target asymmetry F in the $\vec \gamma \vec p\to\eta p$ reaction up to a center-of-mass energy of W=1.9 GeV. The data were obtained with the Crystal-Ball/TAPS detector setup at the Glasgow tagged photon facility of the Mainz Microtron MAMI. All existing model predictions fail to reproduce the new data indicating a significant impact on our understanding of the underlying dynamics of $\eta$ meson photoproduction. The peculiar nodal structure observed in existing T data close to threshold is not confirmed.

PhysicsParticle physicsPhotonProtonMesonNuclear Theorymedia_common.quotation_subjectPartial wave analysisNuclear TheoryGeneral Physics and AstronomyAsymmetryHigh Energy Physics - ExperimentNuclear physicsbeam-target asymmetry F; γ⃗ p⃗ →ηp reaction; Mainz Microtron MAMIHigh Energy Physics::ExperimentNucleonNuclear ExperimentMicrotronNuclear ExperimentCrystal Ballmedia_common
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Nucleon resonance contributions to unpolarised inclusive electron scattering

2019

The first CLAS12 experiments will provide high-precision data on inclusive electron scattering observables at a photon virtuality Q2 ranging from 0.05 to 12GeV2 and center-of-mass energies W up to 4 GeV. In view of this endeavor, we present the modeling of the resonant contributions to the inclusive electron scattering observables. As input, we use the existing CLAS electrocoupling results obtained from exclusive meson electroproduction data off protons, and evaluate for the first time the resonant contributions based on the experimental results on the nucleon resonance electroexcitation. The uncertainties are given by the data and duly propagated through a Monte Carlo approach. In this way…

PhysicsParticle physicsPhotondeep inelastic scattering; proton structureNuclear TheoryMeson010308 nuclear & particles physicsMonte Carlo methodNuclear TheoryFOS: Physical sciencesPartonObservable01 natural sciencesNuclear Theory (nucl-th)High Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)deep inelastic scattering0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsNucleonNuclear ExperimentNuclear theoryElectron scatteringproton structure
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The scale dependent nuclear effects in parton distributions for practical applications

1999

The scale dependence of the ratios of parton distributions in a proton of a nucleus $A$ and in the free proton, $R_i^A(x,Q^2)=f_{i/A}(x,Q^2)/f_i(x,Q^2)$, is studied within the framework of the lowest order leading-twist DGLAP evolution. By evolving the initial nuclear distributions obtained with the GRV-LO and CTEQ4L sets at a scale $Q_0^2$, we show that the ratios $R_i^A(x,Q^2)$ are only moderately sensitive to the choice of a specific modern set of free parton distributions. We propose that to a good first approximation, this parton distribution set-dependence of the nuclear ratios $R_i^A(x,Q^2)$ can be neglected in practical applications. With this result, we offer a numerical parametriz…

PhysicsParticle physicsPhysics and Astronomy (miscellaneous)ProtonNuclear TheoryFOS: Physical sciencesDrell–Yan processOrder (ring theory)Scale (descriptive set theory)PartonNuclear Theory (nucl-th)Nuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Distribution (mathematics)DGLAPEngineering (miscellaneous)Parametrization
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