Search results for "Physics::Accelerator Physics"

showing 10 items of 1235 documents

T2K neutrino flux prediction

2013

The Tokai-to-Kamioka (T2K) experiment studies neutrino oscillations using an off-axismuon neutrino beam with a peak energy of about 0.6 GeV that originates at the Japan Proton Accelerator Research Complex accelerator facility. Interactions of the neutrinos are observed at near detectors placed at 280 m from the production target and at the far detector-Super-Kamiokande-located 295 km away. The flux prediction is an essential part of the successful prediction of neutrino interaction rates at the T2K detectors and is an important input to T2K neutrino oscillation and cross section measurements. A FLUKA and GEANT3-based simulation models the physical processes involved in the neutrino producti…

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsSolar neutrinoAstrophysics::High Energy Astrophysical Phenomenaddc:500.2Antiprotons01 natural sciences7. Clean energyHigh Energy Physics - ExperimentNuclear physicsPions0103 physical sciencesMomentum rangeMuon neutrino010306 general physicsNeutrino oscillationNuclear ExperimentQCPhysicsGev-c010308 nuclear & particles physicsParticle-productionHigh Energy Physics::PhenomenologyT2K experimentFísicaDetectorMonitorSolar neutrino problemNucleiNeutrino detector13. Climate actionMeasurements of neutrino speedPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNeutrinoProtonsAbsorption cross-sectionsParticle Physics - Experiment
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Study of energy response and resolution of the ATLAS barrel calorimeter to hadrons of energies from 20 to 350 GeV

2010

A fully instrumented slice of the ATLAS detector was exposed to test beams from the SPS (Super Proton Synchrotron) at CERN in 2004. In this paper, the results of the measurements of the response of the barrel calorimeter to hadrons with energies in the range 20 to 350 GeV and beam impact points and angles corresponding to pseudorapidity values in the range 0.2-0.65 are reported. The results are compared to the predictions of a simulation program using the Geant 4 toolkit.

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsTest-beamHadronCalorimetry01 natural sciencesNuclear physicsAtlas (anatomy)0103 physical sciencesmedicine[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex][PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsNuclear ExperimentInstrumentationPhysicsRange (particle radiation)Large Hadron ColliderCalorimeter (particle physics)010308 nuclear & particles physicsATLASSuper Proton Synchrotronmedicine.anatomical_structurePseudorapidityCalibrationPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentBeam (structure)Simulation
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Search for Higgs boson production in trilepton and like-charge electron-muon final states with the D0 detector

2013

We present a search for Higgs bosons in multilepton final states in pp-bar collisions at sqrt(s)=1.96 TeV recorded with the D0 detector at the Fermilab Tevatron Collider, using the full Run II data set with integrated luminosities of up to 9.7 fb-1. The multilepton states considered are two electron plus muon, electron with two muons, muon with two hadronic tau leptons, and like-charge electron-muon pairs. These channels directly probe the HVV (V=W,Z) coupling of the Higgs boson in production and decay. The muon with two hadronic tau lepton channel is also sensitive to H to tau lepton pair decays. Upper limits at the 95% C.L on the rate of standard model Higgs boson production are derived i…

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsTevatronFOS: Physical sciences7. Clean energy01 natural scienceslaw.inventionStandard ModelHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsColliderBosonPhysicsMuon010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGHiggs bosonPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentLepton
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Particle Production in the Color Class Condensate: from electron-proton DIS to proton-nucleus collisions

2013

We study single inclusive hadron production in proton-proton and proton-nucleus collisions in the CGC framework. The parameters in the calculation are obtained by fitting electron-proton deep inelastic scattering data. The obtained dipole-proton amplitude is generalized to dipole-nucleus scattering without any additional nuclear parameters other than the Woods-Saxon distribution. We show that it is possible to use an initial condition without an anomalous dimension and still obtain a good description of the HERA inclusive cross section and LHC single particle production measurements. We argue that one must consistently use the proton transverse area as measured by a high virtuality probe in…

Nuclear and High Energy PhysicsParticle physicsProtonNuclear TheoryHadronNuclear TheoryFOS: Physical sciences01 natural sciences7. Clean energyColor-glass condensateNuclear physicsNuclear Theory (nucl-th)Cross section (physics)High Energy Physics - Phenomenology (hep-ph)0103 physical sciences010306 general physicsNuclear ExperimentPhysicsLarge Hadron Colliderta114010308 nuclear & particles physicsScatteringHERADeep inelastic scatteringHigh Energy Physics - PhenomenologyPhysics::Accelerator Physics
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A collision timing monitor for SuperKEKB

2017

Abstract The analysis of beamstrahlung radiation, emitted from a beam of charged particles due to the electromagnetic interaction with a second beam of charged particles, provides a diagnostic tool that can be used to monitor beam–beam collisions in a e + e − storage ring. In this paper we show that the beamstrahlung time profile is related to the timing of the collisions and the length of the beams, and how its measurement can be used to monitor and optimize collisions at the interaction point of the SuperKEKB collider. The method has a unique passive monitor capability, since it allows to monitor the timing of the collision without disturbing (scanning) the beam–beam timing, which needs t…

Nuclear and High Energy PhysicsPhotonBeamstrahlungRadiationUp-conversion01 natural scienceslaw.inventionOpticslaw0103 physical sciencesFrequency-mixing010306 general physicsColliderInstrumentationPhysicsInteraction point010308 nuclear & particles physicsbusiness.industryCollision-timingCharged particleBunchesNon-linear-crystalPhysics::Accelerator PhysicsbusinessStorage ringBeam (structure)Beam-monitoring
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Electron and Photon Identification in the D0 Experiment

2013

The electron and photon reconstruction and identification algorithms used by the D0 Collaboration at the Fermilab Tevatron collider are described. The determination of the electron energy scale and resolution is presented. Studies of the performance of the electron and photon reconstruction and identification are summarized.

Nuclear and High Energy PhysicsPhotonMonte Carlo methodTevatronFOS: Physical sciencesElectron01 natural sciencesHigh Energy Physics - Experimentlaw.inventionNuclear physicsHigh Energy Physics - Experiment (hep-ex)law0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Fermilab010306 general physicsColliderInstrumentationPhysics010308 nuclear & particles physicsResolution (electron density)D0 experiment3. Good healthExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGPhysics::Accelerator PhysicsHigh Energy Physics::Experiment
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Performance and characterization of the FinEstBeAMS beamline at the MAX IV Laboratory

2021

European Regional Development Fund (grant No. TK-141 HiTechDevices 2014-2020.4.01.15-0011 to University of Tartu; grant No. MAX-TEENUS 2014-2020.4.01.20-0278 to University of Tartu; grant No. Eesti Kiirekanal SLOFY11156T/1 to University of Tartu); Estonian Research Council (grant No. PRG-629 to University of Tartu); Jane & Aatos Erkko Foundation (grant No. SOFUS); Business Finland (grant No. 1464/31/2019); Academy of Finland (grant No. 319042; grant No. 326461; grant No. 326406; grant No. 320165); University of Oulu; University of Turku; Tampere University; University of Tartu.

Nuclear and High Energy PhysicsPhotonPhysics::Instrumentation and Detectorsphoton energy resolutionPhysics::Optics02 engineering and technologyPhoton energyGrating114 Physical sciences01 natural scienceslaw.inventionOpticslaw0103 physical sciencesno topic specified010306 general physicsInstrumentationMonochromatorPhysicsRadiationbusiness.industryBeamlinesMAX IVUndulator021001 nanoscience & nanotechnologyphoton fluxSynchrotronplane grating monochromatorBeamline:NATURAL SCIENCES [Research Subject Categories]Physics::Accelerator Physicsbeam polarization0210 nano-technologybusinessStorage ringJournal of Synchrotron Radiation
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A short-orbit spectrometer for low-energy pion detection in electroproduction experiments at MAMI

2017

A new Short-Orbit Spectrometer (SOS) has been constructed and installed within the experimental facility of the A1 collaboration at Mainz Microtron (MAMI), with the goal to detect low-energy pions. It is equipped with a Browne-Buechner magnet and a detector system consisting of two helium-ethane based drift chambers and a scintillator telescope made of five layers. The detector system allows detection of pions in the momentum range of 50 - 147 MeV/c, which corresponds to 8.7 - 63 MeV kinetic energy. The spectrometer can be placed at a distance range of 54 - 66 cm from the target center. Two collimators are available for the measurements, one having 1.8 msr aperture and the other having 7 ms…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsAperturePhysics::Instrumentation and DetectorsFOS: Physical sciencesScintillatorKinetic energy01 natural scienceslaw.inventionNuclear physicsTelescopePionlaw0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentInstrumentationMicrotronPhysicslow-energy pion detectionSpectrometer010308 nuclear & particles physicsDetectorInstrumentation and Detectors (physics.ins-det)3. Good healthPhysics::Accelerator Physics
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A linear radiofrequency ion trap for accumulation, bunching, and emittance improvement of radioactive ion beams

2000

An ion beam cooler and buncher has been developed for the manipulation of radioactive ion beams. The gas-filled linear radiofrequency ion trap system is installed at the Penning trap mass spectrometer ISOLTRAP at ISOLDE/CERN. Its purpose is toaccumulate the 60-keV continuous ISOLDE ion beam with high efficiency and to convert it into low-energy low-emittance ion pulses. The efficiency was found to exceed 10\,\% in agreement with simulations. A more than 10-fold reduction of the ISOLDE beam emittance can be achieved. The system has been used successfully for first on-line experiments. Its principle, setup and performance will be discussed. An ion beam cooler and buncher has been developed fo…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsIon beamIon trapFOS: Physical sciencesMass spectrometryIon cooling01 natural sciencesISOLTRAPIonNuclear physics0103 physical sciencesThermal emittance[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Nuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentInstrumentationNuclear ExperimentRadioactive ion beamsIon guide21.10.Dr; 2.10.Bi; 07.75.+hPhysicsOn-line mass spectrometry010308 nuclear & particles physicsInstrumentation and Detectors (physics.ins-det)Penning trapAccelerators and Storage RingsIon buncherPhysics::Accelerator PhysicsIon trapBeam emittance
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Measurements of the T2K neutrino beam properties using the INGRID on-axis near detector

2012

Precise measurement of neutrino beam direction and intensity was achieved based on a new concept with modularized neutrino detectors. INGRID (Interactive Neutrino GRID) is an on-axis near detector for the T2K long baseline neutrino oscillation experiment. INGRID consists of 16 identical modules arranged in horizontal and vertical arrays around the beam center. The module has a sandwich structure of iron target plates and scintillator trackers. INGRID directly monitors the muon neutrino beam profile center and intensity using the number of observed neutrino events in each module. The neutrino beam direction is measured with accuracy better than 0.4 mrad from the measured profile center. The …

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsNeutrino oscillationPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical Phenomenaon-axis near detectorFOS: Physical sciencesddc:500.201 natural sciences7. Clean energyNeutrino oscillation; on-axis near detectorneutrino oscillation; neutrino detector; wavelength shifting fiber; t2k; extruded scintillator; neutrino beamNeutrino detectorNuclear physicsNeutrino beamneutrino beam0103 physical sciencesExtruded scintillatorMuon neutrinoneutrino oscillation[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsNeutrino oscillationInstrumentationT2KPhysicst2k010308 nuclear & particles physicsHigh Energy Physics::PhenomenologyNeutrino oscillation; T2K; Neutrino beam; Neutrino detector; Extruded scintillator; Wavelength shifting fiberT2K experimentextruded scintillatorFísicaInstrumentation and Detectors (physics.ins-det)Neutrino detectorneutrino detectorWavelength shiftingfiberMeasurements of neutrino speedPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNeutrinoBeam (structure)Leptonwavelength shifting fiber
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