0000000000476889

AUTHOR

R. Snopkov

showing 4 related works from this author

Performance of the ATLAS liquid argon endcap calorimeter in the pseudorapidity region in beam tests

2008

Abstract The pseudorapidity region 2.5 | η | 4.0 in ATLAS is a particularly complex transition zone between the endcap and forward calorimeters. A set-up consisting of 1 4 resp. 1 8 of the full azimuthal acceptance of the ATLAS liquid argon endcap and forward calorimeters has been exposed to beams of electrons, pions and muons in the energy range E ⩽ 200 GeV at the CERN SPS. Data have been taken in the endcap and forward calorimeter regions as well as in the transition region. This beam test set-up corresponds very closely to the geometry and support structures in ATLAS. A detailed study of the performance in the endcap and forward calorimeter regions is described. The data are compared wit…

PhysicsNuclear and High Energy PhysicsParticle physicsMuonLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physics01 natural sciencesCalorimeterNuclear physicsmedicine.anatomical_structurePionAtlas (anatomy)Pseudorapidity0103 physical sciencesmedicineCathode rayHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Hadronic calibration of the ATLAS liquid argon end-cap calorimeter in the pseudorapidity region in beam tests

2004

Abstract A full azimuthal φ -wedge of the ATLAS liquid argon end-cap calorimeter has been exposed to beams of electrons, muons and pions in the energy range 6 GeV ⩽ E ⩽ 200 GeV at the CERN SPS. The angular region studied corresponds to the ATLAS impact position around the pseudorapidity interval 1.6 | η | 1.8 . The beam test setup is described. A detailed study of the performance is given as well as the related intercalibration constants obtained. Following the ATLAS hadronic calibration proposal, a first study of the hadron calibration using a weighting ansatz is presented. The results are compared to predictions from Monte Carlo simulations, based on GEANT 3 and GEANT 4 models.

GEANT-3PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsMonte Carlo methodHadron01 natural sciences7. Clean energyCalorimeterNuclear physicsmedicine.anatomical_structureAtlas (anatomy)Pseudorapidity0103 physical sciencesmedicineHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Liquid argon calorimeter performance at high rates

2012

Abstract We project the performance of the ATLAS liquid argon endcap and forward calorimeters at the planned high luminosity LHC option HL-LHC by exposing small calorimeter modules of the electromagnetic, hadronic, and forward calorimeters to high intensity beams at IHEP/Protvino. The beam intensity extends well beyond the maximum expected for these calorimeters at HL-LHC. The signal reconstruction and calorimeter performance have been studied in full detail.

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderArgonLuminosity (scattering theory)Physics::Instrumentation and Detectorschemistry.chemical_elementCryogenicsCalorimeterNuclear physicsmedicine.anatomical_structurechemistryAtlas (anatomy)medicineMeasuring instrumentPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentInstrumentationBeam (structure)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Hadron energy reconstruction for the ATLAS calorimetry in the framework of the non-parametrical method

2002

This paper discusses hadron energy reconstruction for the ATLAS barrel prototype combined calorimeter (consisting of a lead-liquid argon electromagnetic part and an iron-scintillator hadronic part) in the framework of the non-parametrical method. The non-parametrical method utilizes only the known $e/h$ ratios and the electron calibration constants and does not require the determination of any parameters by a minimization technique. Thus, this technique lends itself to an easy use in a first level trigger. The reconstructed mean values of the hadron energies are within $\pm 1%$ of the true values and the fractional energy resolution is $[(58\pm3)% /\sqrt{E}+(2.5\pm0.3)%]\oplus (1.7\pm0.2)/E…

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsHadronFOS: Physical scienceschemistry.chemical_elementCalorimetryElectronCalorimetry01 natural sciencesPartícules (Física nuclear)High Energy Physics - ExperimentEnergy measurementNuclear physicsHigh Energy Physics - Experiment (hep-ex)PionShower counter0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Computer data analysis[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Combined calorimeterDetectors and Experimental Techniques010306 general physicsNuclear ExperimentInstrumentationPhysicsLarge Hadron ColliderArgon010308 nuclear & particles physicsSHOWER DEVELOPMENT; RESOLUTIONSHOWER DEVELOPMENTCalorimeterRESOLUTIONchemistryScintillation counterHigh Energy Physics::ExperimentCompensation
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