Search results for "Muon Spectrometer"

showing 7 items of 7 documents

Search for long-lived particles produced in pp collisions at s=13  TeV that decay into displaced hadronic jets in the ATLAS muon spectrometer

2019

A search for the decay of neutral, weakly interacting, long-lived particles using data collected by the ATLAS detector at the LHC is presented. The analysis in this paper uses 36.1 fb(-1) of proton ...

PhysicsLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAtlas (topology)Atlas detectorHadronAtlas muon spectrometer01 natural sciencesNuclear physicsMuon spectrometer0103 physical sciencesHiggs bosonHigh Energy Physics::Experiment010306 general physicsPhysical Review D
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Resolution of the ATLAS muon spectrometer monitored drift tubes in LHC Run 2

2019

The momentum measurement capability of the ATLAS muon spectrometer relies fundamentally on the intrinsic single-hit spatial resolution of the monitored drift tube precision tracking chambers. Optimal resolution is achieved with a dedicated calibration program that addresses the specific operating conditions of the 354 000 high-pressure drift tubes in the spectrometer. The calibrations consist of a set of timing offsets and drift time to drift distance transfer relations, and result in chamber resolution functions. This paper describes novel algorithms to obtain precision calibrations from data collected by ATLAS in LHC Run 2 and from a gas monitoring chamber, deployed in a dedicated gas fac…

Wire chambers (MWPCdrift tube13000 GeV-cmsPhysics::Instrumentation and DetectorsmuonsTracking (particle physics)01 natural sciences030218 nuclear medicine & medical imagingHigh Energy Physics - ExperimentSubatomär fysikMWPCHigh Energy Physics - Experiment (hep-ex)Gaseous detectors0302 clinical medicineWire chambersDrift tubesSubatomic Physicsscattering [p p][PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]tracking detectorProportional chambersmomentum resolutionInstrumentationImage resolutionMathematical Physicsdrift tubesPhysicsLarge Hadron ColliderDrift chamberstrack data analysisMuon spectrometersResolution (electron density)DetectorSettore FIS/01 - Fisica SperimentaleATLAS:Mathematics and natural scienses: 400::Physics: 430::Nuclear and elementary particle physics: 431 [VDP]Wire chambers (MWPC Thin-gap chambers drift chambers drift tubes proportional chambers etc)medicine.anatomical_structureCERN LHC Collproportional chambers etc)Gaseous detectors; Muon spectrometers; Particle tracking detectors (gaseous detectors); Wire chambers (MWPC thin-gap chambers drift chambers drift tubes proportional chambers etc)MDT chambersWire chambers (MWPC)LHCcolliding beams [p p]Particle Physics - Experimentp p: scatteringspectrometer [muon]Ciências Naturais::Ciências Físicas530 PhysicsParticle tracking detectors (Gaseous detectors):Ciências Físicas [Ciências Naturais]610FOS: Physical sciencesdrift chamber [muon]gas [monitoring]programming03 medical and health sciencesOpticsAtlas (anatomy)Muon spectrometer0103 physical sciencesCalibrationmedicinemuon: drift chamberGaseous detectorddc:610drift chambersHigh Energy Physicsspatial resolutionMuonScience & Technology010308 nuclear & particles physicsbusiness.industryhep-ex:Matematikk og naturvitenskap: 400::Fysikk: 430::Kjerne- og elementærpartikkelfysikk: 431 [VDP]Thin-gap chamberscalibrationmonitoring: gasExperimental High Energy Physicsbusinessp p: colliding beamsmuon: spectrometerexperimental results
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Algorithms for the ROD DSP of the ATLAS Hadronic Tile Calorimeter

2007

In this paper we present the performance of two algorithms currently running in the Tile Calorimeter Read-Out Driver boards for the commissioning of ATLAS. The first algorithm presented is the so called Optimal Filtering. It reconstructs the deposited energy in the Tile Calorimeter and the arrival time of the data. The second algorithm is the MTag which tags low transverse momentum muons that may escape the ATLAS muon spectrometer first level trigger. Comparisons between online (inside the Read-Out Drivers) and offline implementations are done with an agreement around 99% for the reconstruction of the amplitude using the Optimal Filtering algorithm and a coincidende of 93% between the offli…

MuonPhysics::Instrumentation and Detectorsbusiness.industryAtlas (topology)Computer scienceHadronAtlas muon spectrometerTile calorimeterAmplitudeLevel triggerbusinessInstrumentationAlgorithmMathematical PhysicsDigital signal processing
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ϒ production and nuclear modification at forward rapidity in Pb–Pb collisions at sNN=5.02TeV

2021

Abstract The production of ϒ mesons in Pb–Pb collisions at a centre-of-mass energy per nucleon pair s NN = 5.02 TeV is measured with the muon spectrometer of the ALICE detector at the LHC. The yields as well as the nuclear modification factors are determined in the forward rapidity region 2.5 y 4.0 , as a function of rapidity, transverse momentum and collision centrality. The results show that the production of the ϒ ( 1S ) meson is suppressed by a factor of about three with respect to the production in proton–proton collisions. For the first time, a significant signal for the ϒ ( 2S ) meson is observed at forward rapidity, indicating a suppression stronger by about a factor 2–3 with respec…

PhysicsNuclear and High Energy PhysicsLarge Hadron ColliderMeson010308 nuclear & particles physicsNuclear TheoryCollision7. Clean energy01 natural sciencesNuclear physicsMuon spectrometer0103 physical sciencesTransverse momentumHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsGround stateNucleonPhysics Letters B
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Search for heavy long-lived charged particles with the ATLAS detector in pp collisions at root s=7 TeV

2011

A search for long-lived charged particles reaching the muon spectrometer is performed using a data sample of 37 pb[superscript −1] from pp collisions at √s = 7 TeV collected by the ATLAS detector at the LHC in 2010. No excess is observed above the estimated background. Stable [~ over τ] sleptons are excluded at 95% CL up to a mass of 136 GeV, in GMSB models with N[subscript 5] = 3, mmessenger = 250 TeV, sign(μ) = 1 and tanβ = 5. Electroweak production of sleptons is excluded up to a mass of 110 GeV. Gluino R-hadrons in a generic interaction model are excluded up to masses of 530 GeV to 544 GeV depending on the fraction of R-hadrons produced as [~ over g]-balls.

Nuclear and High Energy PhysicsParticle physicsAtlas detectorCiências Naturais::Ciências FísicasPhysics::Instrumentation and Detectors:Ciências Físicas [Ciências Naturais]FOS: Physical sciencesddc:500.2SUSY; ATLAS; Long-lived particles01 natural sciences530CHARGED PARTICLESHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Muon spectrometerAtlas (anatomy)0103 physical sciencesmedicine[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]ddc:530High Energy Physics010306 general physicsNuclear ExperimentPhysicsScience & TechnologyATLAS detector010308 nuclear & particles physicsHigh Energy Physics::PhenomenologySettore FIS/01 - Fisica SperimentaleFísicaSUSYSupersymmetryATLASCharged particleLong-lived particlesmedicine.anatomical_structureHADRON-HADRON COLLISIONSR-hadronExperimental High Energy PhysicsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGFísica nuclearHigh Energy Physics::ExperimentLHCsupersymmetryParticle Physics - Experiment
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Forward-central two-particle correlations in p–Pb collisions at sNN=5.02 TeV

2016

Two-particle angular correlations between trigger particles in the forward pseudorapidity range (2.5 < |η| < 4.0) and associated particles in the cen

Physicscongenital hereditary and neonatal diseases and abnormalitiesNuclear and High Energy PhysicsParticle physicsTime projection chamber010308 nuclear & particles physicsAtlas detector01 natural sciencesCharged particleNuclear physicsMuon spectrometerPseudorapidity0103 physical sciencesTransverse momentumRapidityMultiplicity (chemistry)010306 general physicsPhysics Letters B
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Commissioning of the ATLAS Muon Spectrometer with cosmic rays

2010

The ATLAS detector at the Large Hadron Collider has collected several hundred million cosmic ray events during 2008 and 2009. These data were used to commission the Muon Spectrometer and to study the performance of the trigger and tracking chambers, their alignment, the detector control system, the data acquisition and the analysis programs. We present the performance in the relevant parameters that determine the quality of the muon measurement. We discuss the single element efficiency, resolution and noise rates, the calibration method of the detector response and of the alignment system, the track reconstruction efficiency and the momentum measurement. The results show that the detector i…

SystemAstrofísicaDriftPhysics - Instrumentation and DetectorsMuon SpectrometerPhysics and Astronomy (miscellaneous)Physics::Instrumentation and DetectorsTracking (particle physics)01 natural sciences7. Clean energyHigh Energy Physics - ExperimentDrift TubeMDTHigh Energy Physics - Experiment (hep-ex)Data acquisitionATLAS muon spectrometer[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental TechniquesNuclear ExperimentPhysicsLarge Hadron Collidercosmic ray eventsDetectorSettore FIS/01 - Fisica SperimentaleBeamInstrumentation and Detectors (physics.ins-det)ATLASmedicine.anatomical_structureTrack ReconstructionPhysical SciencesFísica nuclearLHCmuon measurementFOS: Physical sciencesCosmic rayddc:500.2530Nuclear physicsAtlas (anatomy)0103 physical sciencesCalibrationmedicineFysikddc:530High Energy Physics[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsEngineering (miscellaneous)Ciencias ExactasMuonChambersMuon TrackCosmologiaATLAS detector010308 nuclear & particles physicsFísicaTrack SegmentPhysics::Accelerator Physicsproton-proton collisionsHigh Energy Physics::Experiment
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