Search results for "Experimental technique"

showing 10 items of 227 documents

New methods of evaluation of the flavor composition in e+ e- annihilation by double hemisphere tagging at LEP / SLC energies

1995

Two new methods are proposed to extract the flavour contents of the events produced at LEP/SLC, together with the classification matrix of a tagging by hemispheres. By utilising the tagging obtained in both hemispheres, the efficiencies, backgrounds and flavour compositions are directly obtained by fitting the data. A minimal dependence on modelling and a consistent treatment of systematic errors are achieved by applying these methods. The choice of the tagging algorithm is irrelevant in the methods, provided that similar efficiencies are reached. As an example, a multivariate analysis technique combining the tracking information given by a microvertex detector has been applied to extract t…

PhysicsSystematic errorNuclear and High Energy PhysicsAnnihilationBranching fractionFlavourDetectorHigh Energy Physics::PhenomenologyComposition (combinatorics)Tracking (particle physics)Nuclear physicsMatrix (mathematics)Física nuclearHigh Energy Physics::ExperimentDetectors and Experimental TechniquesInstrumentation
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The RICH counter in the CERN hyperon beam experiment

1992

Abstract The hyperon beam experiment WA89 at the CERN-SPS uses a ring imaging Cherenkov counter (RICH) for identification of secondaries from ∑ − N reactions. Cherenkov photons are generated in a 5 m long radiator volume filled with nitrogen at atmospheric pressure and detected in drift chambers. The drift chambers cover an active surface of 1.6 × 0.75 m 2 , with a maximum drift path of 41 cm. Photoelectrons are counted on 1280 wires with a pitch of 2.54 mm, equipped with multihit TDCs. The counting gas is ethane saturated with TMAE at 30°C. The counter was operated in two beam periods in 1990 and 1991. The spatial resolution of the chambers is better than 2 mm and under normal running cond…

PhysicsWire chamberNuclear and High Energy PhysicsPhotonLarge Hadron ColliderAtmospheric pressurePhysics::Instrumentation and DetectorsHyperonPhotoelectric effectCharged particleParticle detectorNuclear physicsVolume (thermodynamics)Measuring instrumentHigh Energy Physics::ExperimentDetectors and Experimental TechniquesAtomic physicsInstrumentationCherenkov radiationBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Combined performance studies for electrons at the 2004 ATLAS combined test-beam

2010

In 2004 at the ATLAS (A Toroidal LHC ApparatuS) combined test beam, one slice of the ATLAS barrel detector (including an Inner Detector set-up and the Liquid Argon calorimeter) was exposed to particles from the H8 SPS beam line at CERN. It was the first occasion to test the combined electron performance of ATLAS. This paper presents results obtained for the momentum measurement p with the Inner Detector and for the performance of the electron measurement with the LAr calorimeter (energy E linearity and resolution) in the presence of a magnetic field in the Inner Detector for momenta ranging from 20 GeV/c to 100 GeV/c. Furthermore the particle identification capabilities of the Transition Ra…

Physics::Instrumentation and DetectorsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]Transition radiation detectorsElectronsddc:500.201 natural sciencesParticle identificationNuclear physicsCalorimetersAtlas (anatomy)Particle tracking detectors0103 physical sciencesmedicine[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental Techniques010306 general physicsNuclear ExperimentInstrumentationDetectors de radiacióMathematical PhysicsPhysicsLarge Hadron ColliderScience & Technology010308 nuclear & particles physicsLarge detector systems for particle and astroparticle physicsDetectorCalorimetermedicine.anatomical_structureTransition radiationBeamlineHigh Energy Physics::ExperimentBeam (structure)
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Future Linear Colliders: Detector R&D, Jet Reconstruction and Top Physics Potential

2016

RESUMEN: Durante el siglo XX, los descubrimientos de nuevas partículas y las medidas realizadas en los colisionadores, junto con el progreso de la física teórica, nos permitieron formular el Modelo Estándar (SM) de las interacciones entre los constituyentes de la materia. El descubrimiento del bosón de Higgs en el LHC fue un gran paso en nuestra compren- sión de las interacciones fundamentales de la naturaleza y la estructura de la materia descrita por el Modelo Estándar. Con el fin de establecer el mecanismo de ruptura de simetría electrodébil, todas las propiedades del bosón de Higgs (masa, acoplamientos, amplitud de desintegración, espín) deben medirse con precisión. El LHC tiene excelen…

Physics::Instrumentation and Detectorsfuture linear collidersPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentDetectors and Experimental Techniquestop quarkjet reconstructionParticle Physics - Experimentdetector R&D
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A dynamic model for hysteresis in magnetostrictive devices

2014

In this paper, a dynamic model for the description and design of hysteresis in magnetostrictive devices is presented. The model is based on Preisach theory and its dynamic extension. A procedure for determining the Preisach distribution function is given. This procedure is based on neural networks. The model is able to reconstruct both the magnetization relation and the field-strain relation. The model is validated through comparison and prediction of data collected from a typical Terfenol-D sample and a novel experimental technique dedicated to the validation of dynamic models is proposed.

Preisach distribution functionRelation (database)Artificial neural networkComputer scienceExperimental techniqueGeneral Physics and AstronomyMagnetostrictionMagnetic hysteresisHysteresisDistribution functionTerfenol-DPreisach theoryControl theoryDynamic ExtensionHysteresiMagnetostrictive devices Dynamic extensionTerfenol-DJournal of Applied Physics
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The Next Generation of Axion Helioscopes: The International Axion Observatory (IAXO)

2015

Çetin, Serkant Ali (Dogus Author) -- Conference full title: 13th International Conference on Topics in Astroparticle and Underground Physics, TAUP 2013; Asilomar Conference Grounds Monterey Peninsula; United States; 8 September 2013 through 13 September 2013. The International Axion Observatory (IAXO) is a proposed 4th-generation axion helioscope with the primary physics research goal to search for solar axions via their Primakoff conversion into photons of 1 - 10 keV energies in a strong magnetic field. IAXO will achieve a sensitivity to the axion-photon coupling gaγ down to a few ×10-12 GeV-1 for a wide range of axion masses up to ∼ 0.25 eV. This is an improvement over the currently best …

QCD axionParticle physicsPhysics::Instrumentation and DetectorsDark matterPhysics and Astronomy(all)01 natural sciences7. Clean energymagnetic helioscopeHigh Energy Physics::TheoryQCD axionsAstroparticle PhysicsAxionObservatory0103 physical sciencesDark matterQCD axions; magnetic helioscope; dark matterDark Matterddc:530Detectors and Experimental Techniques010306 general physicsAxionAstroparticle physicsPhysicsHelioscope010308 nuclear & particles physicsAxion Dark Matter ExperimentHigh Energy Physics::PhenomenologyStrong CP problemIAXOStrong CP ProblemALPStrong CP problemAstroparticle physicsCERN Axion Solar TelescopeParticle Physics - ExperimentHelioscopesPhysics Procedia
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Top physics studies at the LHC in the standard model and beyond with the ATLAS detector

2009

The LHC will be a Top quark factory, producing large numbers of Top quarks even at the initial low luminosities. This will enable a rich program of Top quark Physics to be explored, both within the Standard Model and using Top quarks as probes of Physics Beyond the Standard Model. Recent studies from ATLAS will be presented, including prospects for the measurements of the production of Top pairs and single Top production, angular correlations in the Top decay, and the precision measurement of the Top quark mass. The search for Physics beyond the Standard Model will be illustrated with searches for rare Top decays involving Flavour Changing Neutral Currents, and the reconstruction of tt-bar …

QuarkPhysicsHistoryTop quarkParticle physicsLarge Hadron Collider010308 nuclear & particles physicsPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyFlavourTop quark condensateOmega baryon01 natural sciencesComputer Science::Computers and SocietyComputer Science ApplicationsEducationSigma baryonNonlinear Sciences::Chaotic DynamicsNuclear physicsNonlinear Sciences::Exactly Solvable and Integrable Systems0103 physical sciencesPhysics::Atomic and Molecular ClustersHigh Energy Physics::ExperimentDetectors and Experimental Techniques010306 general physicsJournal of Physics: Conference Series
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Top mass reconstruction in ATLAS

2011

The top-quark mass is a fundamental parameter of the Standard Model. After the discovery of the top quark, the measurements of its properties were of substantial interest. Within the framework of the SM, the top-quark mass can be used in combination with other electroweak precision measurements to constrain the mass of the yet unobserved Higgs boson.\nIn the new era of the Large Hadron Collider (LHC), the first top quarks have been produced in Europe in proton-proton collisions at a center-of-mass energy of 7~TeV. The top-quark mass measurement of ATLAS in the so called lepton+jets channel with 35~pb$^{-1}$ integrated luminosity will be presented. In this early data-taking period the larges…

QuarkPhysicsHistoryTop quarkParticle physicsLarge Hadron ColliderHigh Energy Physics::LatticeNuclear TheoryHigh Energy Physics::PhenomenologyElectroweak interactionTechnicolorTop quark condensateComputer Science ApplicationsEducationNuclear physicsPhysics::Atomic and Molecular ClustersHiggs bosonHigh Energy Physics::ExperimentDetectors and Experimental TechniquesLeptonJournal of Physics: Conference Series
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The SPEDE spectrometer

2017

8 pags., 10 figs., 2 tabs.

Radioactive ion beamsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsElectron spectrometerPhysics::Instrumentation and DetectorsFOS: Physical sciencesElectronnucl-ex7. Clean energy01 natural sciencesMomentumNuclear physicsInternal conversion0103 physical sciencesNuclear Physics - ExperimentDetectors and Experimental TechniquesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear Experimentphysics.ins-detPhysicsLarge Hadron ColliderSpectrometer010308 nuclear & particles physicsInstrumentation and Detectors (physics.ins-det)Magnetic fieldPhysics::Accelerator Physics
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A high-resolution PET demonstrator using a silicon "magnifying glass".

2021

Abstract To assist ongoing investigations of the limits of the tradeoff between spatial resolution and noise in PET imaging, several PET instruments based on silicon-pad detectors have been developed. The latest is a segment of a dual-ring device to demonstrate that excellent reconstructed image resolution can be achieved with a scanner that uses highresolution detectors placed close to the object of interest or surrounding a small field-of-view in combination with detectors having modest resolution at larger radius. The outer ring of our demonstrator comprises conventional BGO block detectors scavenged from a clinical PET scanner and located at a 500 mm radius around a 50 mm diameter field…

ScannerPhotonSiliconchemistry.chemical_elementScintillatorPhysics and Astronomy(all)01 natural sciencesArticle030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicineOpticssilicon detectors0103 physical sciencesDetectors and Experimental Techniquesmagnifying PETImage resolutionPhysics010308 nuclear & particles physicsbusiness.industryDetectorResolution (electron density)high-resolution imagingRadiusPETchemistrybusinessPhysics procedia
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