Search results for "Accelerator"

showing 10 items of 1507 documents

"Sigma20" of "Accurate Test of Chiral Dynamics in the \boldmath$\gamma p \rightarrow \pi^0p$ Reaction"

2022

Photon beam asymmetry Sigma at W=1.1137946 GeV

POLPhotoproductionAsymmetry MeasurementAstrophysics::High Energy Astrophysical PhenomenaPolarizationPhysics::OpticsPhysics::Accelerator PhysicsGAMMA P --> PI0 PExclusiveHigh Energy Physics::ExperimentNuclear Experiment
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"Sigma08" of "Accurate Test of Chiral Dynamics in the \boldmath$\gamma p \rightarrow \pi^0p$ Reaction"

2022

Photon beam asymmetry Sigma at W=1.0895214 GeV

POLPhotoproductionAsymmetry MeasurementAstrophysics::High Energy Astrophysical PhenomenaPolarizationPhysics::OpticsPhysics::Accelerator PhysicsGAMMA P --> PI0 PExclusiveHigh Energy Physics::ExperimentNuclear Experiment
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"Sigma09" of "Accurate Test of Chiral Dynamics in the \boldmath$\gamma p \rightarrow \pi^0p$ Reaction"

2022

Photon beam asymmetry Sigma at W=1.0915347 GeV

POLPhotoproductionAsymmetry MeasurementAstrophysics::High Energy Astrophysical PhenomenaPolarizationPhysics::OpticsPhysics::Accelerator PhysicsGAMMA P --> PI0 PExclusiveHigh Energy Physics::ExperimentNuclear Experiment
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"Sigma13" of "Accurate Test of Chiral Dynamics in the \boldmath$\gamma p \rightarrow \pi^0p$ Reaction"

2022

Photon beam asymmetry Sigma at W=1.0996192 GeV

POLPhotoproductionAsymmetry MeasurementAstrophysics::High Energy Astrophysical PhenomenaPolarizationPhysics::OpticsPhysics::Accelerator PhysicsGAMMA P --> PI0 PExclusiveHigh Energy Physics::ExperimentNuclear Experiment
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Determination of beta-delayed neutron emission probability limits of rhodium isotopes by gamma-ray spectroscopy

2019

9 pags., 5 figs., 5 tabs. -- 27th International Nuclear Physics Conference (INPC2019) 29 July - 2 August 2019, Glasgow, UK

PaperHistoryFissionNeutron emissionAstrophysics::High Energy Astrophysical PhenomenaNuclear Theorychemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesEducationNuclear physics0103 physical sciencesGamma spectroscopyNuclear drip lineNuclide010306 general physicsNuclear ExperimentPhysicsIsotope010308 nuclear & particles physics3. Good healthComputer Science Applicationsddc:chemistryPhysics::Accelerator PhysicsBerylliumDelayed neutron
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Combination of Tevatron searches for the standard model Higgs boson in the W+W- decay mode.

2010

11 páginas, 4 figuras, 1 tabla.-- CDF Collaboration: et al.

Particle physicsAstrophysics::High Energy Astrophysical PhenomenaTevatronFOS: Physical sciencesGeneral Physics and AstronomyElementary particleddc:500.2.PARTON DISTRIBUTIONS; HADRON COLLIDERS; QCD; NNLO7. Clean energy01 natural sciences114 Physical sciencesHigh Energy Physics - ExperimentStandard ModelNuclear physicsHigh Energy Physics - Experiment (hep-ex)Particle decay0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Grand Unified TheoryHADRON COLLIDERSFermilabTEVATRONNuclear Experiment010306 general physicsBosonPhysicsHIGGS BOSON010308 nuclear & particles physicsPhysicsHigh Energy Physics::PhenomenologyQCD3. Good healthPARTON DISTRIBUTIONSHiggs bosonCDFPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNNLOAnti-p p: interaction | Higgs particle: search for | gluon gluon: fusion | intermediate boson: fusion | quark antiquark: annihilation | Higgs particle: decay | Higgs particle --> W+ W- | W: pair production | W: leptonic decay | dilepton: final state | jet: multiplicity | cross section: upper limit | mass dependence | Higgs particle: mass | background | DZERO | CDF | Batavia TEVATRON Coll | anti-p p --> Higgs particle anything | anti-p p --> Higgs particle anything intermediate boson anything | anti-p p --> Higgs particle anything quark antiquark anything | 1960 GeV-cmsPhysical review letters
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The COMPASS Setup for Physics with Hadron Beams

2015

The main characteristics of the COMPASS experimental setup for physics with hadron beams are described. This setup was designed to perform exclusive measurements of processes with several charged and/or neutral particles in the final state. Making use of a large part of the apparatus that was previously built for spin structure studies with a muon beam, it also features a new target system as well as new or upgraded detectors. The hadron setup is able to operate at the high incident hadron flux available at CERN. It is characterised by large angular and momentum coverages, large and nearly flat acceptances, and good two and three-particle mass resolutions. In 2008 and 2009 it was successful…

Particle physicsCalorimetry; Data acquisition and reconstruction; Fixed target experiment for hadron spectroscopy; Front-end electronics; Micro Pattern detectors and Drift chambers; Monte-Carlo simulation; RICH; Instrumentation; Nuclear and High Energy PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsHadronFOS: Physical sciencesMonte-Carlo simulation[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Calorimetryacquisition and reconstruction01 natural sciences7. Clean energyMicro Pattern detectors and Drift chambersHigh Energy Physics - ExperimentNuclear physicsMomentumHigh Energy Physics - Experiment (hep-ex)CompassHadron spectroscopy0103 physical sciencesDetectors and Experimental Techniques010306 general physicsRICHInstrumentationFixed target experiment for hadron spectroscopyPhysicsDataLarge Hadron Collider010308 nuclear & particles physicsMicroMegas detectorFront-end electronicsInstrumentation and Detectors (physics.ins-det)Micro Pattern detectorsand Drift chambersData acquisition and reconstructionGas electron multiplierPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentParticle Physics - ExperimentBeam (structure)Front-end electronicMicro Pattern detectors and Drift chamber
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Rates, polarizations, and asymmetries in charmless vector-vector B meson decays

2003

With a sample of approximately 89 million BBbar pairs collected with the BABAR detector, we perform a search for B meson decays into pairs of charmless vector mesons (phi, rho, and K*). We measure the branching fractions, determine the degree of longitudinal polarization, and search for CP violation asymmetries in the processes B->phiK*+, B->phiK*0, B->rho0K*+, and B->rho0rho+. We also set an upper limit on the branching fraction for the decay B->rho0rho0.

Particle physicsMesonBABARElectron–positron annihilationHadronFOS: Physical sciencesGeneral Physics and AstronomyElementary particleResonancePARTICLE PHYSICS; PEP2; BABAR01 natural sciencesNOHigh Energy Physics - ExperimentHigh energy physicHigh Energy Physics - Experiment (hep-ex)Particle decayElectromagnetic calorimeterPolarizationProbability density function0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PEP2B mesonDecay dynamic010306 general physicsPhysicsCalorimeter010308 nuclear & particles physicsBranching fractionCP-ASYMMETRIES VIOLATION SEARCH B->VVColliding beam acceleratorComputer simulationDecay rateMonte Carlo methodCrystallographyPARTICLE PHYSICSCP violationHigh Energy Physics::ExperimentParticle detectorProton
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Observation of Orbitally Excited Bs Mesons

2007

We report the first observation of two narrow resonances consistent with states of orbitally excited (L=1) B_s mesons using 1 fb^{-1} of ppbar collisions at sqrt{s} = 1.96 TeV collected with the CDF II detector at the Fermilab Tevatron. We use two-body decays into K^- and B^+ mesons reconstructed as B^+ \to J/\psi K^+, J/\psi \to \mu^+ \mu^- or B^+ \to \bar{D}^0 \pi^+, \bar{D}^0 \to K^+ \pi^-. We deduce the masses of the two states to be m(B_{s1}) = 5829.4 +- 0.7 MeV/c^2 and m(B_{s2}^*) = 5839.7 +- 0.7 MeV/c^2.

Particle physicsMesonFermilab TevatronPhysics::Instrumentation and DetectorsHadronPhysics MultidisciplinaryFOS: Physical sciencesGeneral Physics and Astronomyddc:500.201 natural sciencesResonanceHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Pion0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]B meson010306 general physicsNuclear ExperimentPhysicsMuonMesons010308 nuclear & particles physicsTwo-body decaysPhysicsHigh Energy Physics::PhenomenologyExcited statesElementary particles14.40.Nd 12.40.YxQuarkoniumPair productionMolecular orbitals_Physics::Accelerator PhysicsHigh Energy Physics::ExperimentCollider Detector at Fermilab
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Upgrade of the ALICE Experiment Letter Of Intent

2014

ALICE (A Large Ion Collider Experiment) is studying the physics of strongly interacting matter, and in particular the properties of the Quark–Gluon Plasma (QGP), using proton–proton, proton–nucleus and nucleus–nucleus collisions at the CERN LHC (Large Hadron Collider). The ALICE Collaboration is preparing a major upgrade of the experimental apparatus, planned for installation in the second long LHC shutdown in the years 2018–2019. These plans are presented in the ALICE Upgrade Letter of Intent, submitted to the LHCC (LHC experiments Committee) in September 2012. In order to fully exploit the physics reach of the LHC in this field, high- precision measurements of the heavy-flavour production…

Particle physicsNuclear and High Energy PhysicsCOLISÕES DE ÍONS PESADOS RELATIVÍSTICOSPhysics::Instrumentation and Detectors[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural scienceslaw.inventionNuclear physicspp collisionALICElawpp collision; TeVheavy-ion experiments0103 physical sciencespp collisions; TeVTeV010306 general physicsColliderNuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)ComputingMilieux_MISCELLANEOUSPhysicsALICE experiment LHC heavy-ion experimentsLarge Hadron ColliderLuminosity (scattering theory)010308 nuclear & particles physicsPhysicsDetectorHigh Energy Physics::PhenomenologyALICE experimentNATURAL SCIENCES. Physics.PRIRODNE ZNANOSTI. Fizika.Detector upgradeUpgradeQuark–gluon plasmaPhysics::Accelerator PhysicsupgradeHigh Energy Physics::ExperimentLHCALICE (propellant)upgrade ; ALICEEvent (particle physics)pp collisionsDetector performance
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