Search results for "Collider"

showing 10 items of 1690 documents

The ATLAS Tile Calorimeter performance at LHC

2013

The Tile Calorimeter (TileCal), the central section of the hadronic calorimeter of the ATLAS experiment, is a key detector component to detect hadrons, jets and taus and to measure the missing transverse energy. Due to the very good muon signal to noise ratio it assists the spectrometer in the identification and reconstruction of muons. TileCal is built of steel and scintillating tiles coupled to optical fibers and read out by photomultipliers. The calorimeter is equipped with systems that allow to monitor and to calibrate each stage of the read-out system exploiting different signal sources: laser light, charge injection and a radiactive source. The performance of the calorimeter has been …

PhysicsNuclear and High Energy PhysicsPhotomultiplierLarge Hadron ColliderCalorimeter (particle physics)Physics::Instrumentation and DetectorsRadioactive sourceATLAS experimentDetectorNuclear physicsmedicine.anatomical_structureTile CalorimeterAtlas (anatomy)medicineCalibrationHadronic CalorimeterHigh Energy Physics::ExperimentDetectors and Experimental TechniquesTileCalInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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ALICE T0 detector

2005

T0-the fast timing and trigger detector for the ALICE experiment at CERN LHC-is described. Performance of the T0 prototype measured with a mixture of 6 GeV/c negative pions and kaons is given. The best time resolution (28 ps r.m.s.) was reached with a radiator diameter matching that of the photocathode. The results for all the tested radiator sizes are considerably better than 50 ps-the minimum requirement for the ALICE experiment.

PhysicsNuclear and High Energy PhysicsPhotomultiplierLarge Hadron ColliderPhysics::Instrumentation and DetectorsCherenkov detectorDetectorPhotocathodelaw.inventionNuclear physicsPionNuclear Energy and EngineeringlawRadiator (engine cooling)High Energy Physics::ExperimentElectrical and Electronic EngineeringALICE (propellant)Nuclear ExperimentIEEE Transactions on Nuclear Science
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Prototyping the PANDA Barrel DIRC

2014

The design of the Barrel DIRC detector for the future PANDA experiment at FAIR contains several important improvements compared to the successful BABAR DIRC, such as focusing and fast timing. To test those improvements as well as other design options a prototype was build and successfully tested in 2012 with particle beams at CERN. The prototype comprises a radiator bar, focusing lens, mirror, and a prism shaped expansion volume made of synthetic fused silica. An array of micro-channel plate photomultiplier tubes measures the location and arrival time of the Cherenkov photons with sub-nanosecond resolution. The development of a fast reconstruction algorithm allowed to tune construction deta…

PhysicsNuclear and High Energy PhysicsPhotomultiplierLarge Hadron ColliderPhysics::Instrumentation and Detectorsbusiness.industryDetectorReconstruction algorithmParticle identificationlaw.inventionLens (optics)OpticslawHigh Energy Physics::ExperimentPrismbusinessInstrumentationCherenkov radiationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Study ofX(3915)→J/ψωin two-photon collisions

2012

We study the process $\gamma \gamma \to J/\psi \omega$ using a data sample of 519.2 $fb^{-1}$ recorded by the BaBar detector at SLAC at the PEP-II asymmetric-energy $e^+ e^-$ collider at center-of-mass energies near the $\Upsilon(nS)$ ($n = 2,3,4$) resonances. We confirm the existence of the charmonium-like resonance X(3915) decaying to $J/\psi \omega$ with a significance of 7.6 standard deviations, including systematic uncertainties, and measure its mass $(3919.4 \pm 2.2 \pm 1.6) MeV/c^2$ and width $(13 \pm 6 \pm 3) MeV$, where the first uncertainty is statistical and the second systematic. A spin-parity analysis supports the assignment $J^P=0^+$ and therefore the ident ification of the si…

PhysicsNuclear and High Energy PhysicsPhoton010308 nuclear & particles physicsBranching fractionResonance01 natural sciencesMeasure (mathematics)law.inventionNuclear physicslawProduct (mathematics)0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsColliderPhysical Review D
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Direct photon production ind+Au collisions atsNN=200GeV

2013

Direct photons have been measured in root s(NN) = 200 GeV d + Au collisions at midrapidity. A wide p(T) range is covered by measurements of nearly real virtual photons (1 < p(T) < 6 GeV/c) and real photons (5 < p(T) < 16 GeV/c). The invariant yield of the direct photons in d + Au collisions over the scaled p + p cross section is consistent with unity. Theoretical calculations assuming standard cold-nuclear-matter effects describe the data well for the entire p(T) range. This indicates that the large enhancement of direct photons observed in Au + Au collisions for 1.0 < p(T) < 2.5 GeV/c is attributable to a source other than the initial-state nuclear effects.

PhysicsNuclear and High Energy PhysicsPhoton010308 nuclear & particles physicsVirtual particle01 natural sciences7. Clean energyPhoton yieldNuclear physics0103 physical sciencesAtomic physicsNuclear Experiment010306 general physicsRelativistic Heavy Ion ColliderPhysical Review C
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Search for low-mass resonances decaying into two jets and produced in association with a photon using pp collisions at s=13 TeV with the ATLAS detect…

2019

A search is performed for localised excesses in dijet mass distributions of low-dijet-mass events produced in association with a high transverse energy photon. The search uses up to 79.8 fb−1 of LHC proton–proton collisions collected by the ATLAS experiment at a centre-of-mass energy of 13 TeV during 2015–2017. Two variants are presented: one which makes no jet flavour requirements and one which requires both jets to be tagged as b-jets. The observed mass distributions are consistent with multi-jet processes in the Standard Model. The data are used to set upper limits on the production cross-section for a benchmark Z′ model and, separately, on generic Gaussian-shape contributions to the mas…

PhysicsNuclear and High Energy PhysicsPhotonLarge Hadron Collider010308 nuclear & particles physicsAtlas detectorAtlas (topology)ATLAS experiment7. Clean energy01 natural sciencesNuclear physicsTransverse plane0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsLow MassPhysics Letters B
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Measurement of prompt photon production in sNN=8.16 TeV p + Pb collisions with ATLAS

2019

The inclusive production rates of isolated, prompt photons in p+Pb collisions at sNN=8.16 TeV are studied with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb −1 recorded in 2016. The cross-section and nuclear modification factor RpPb are measured as a function of photon transverse energy from 20 GeV to 550 GeV and in three nucleon–nucleon centre-of-mass pseudorapidity regions, (−2.83,−2.02) , (−1.84,0.91) , and (1.09,1.90) . The cross-section and RpPb values are compared with the results of a next-to-leading-order perturbative QCD calculation, with and without nuclear parton distribution function modifications, and with expectations b…

PhysicsNuclear and High Energy PhysicsPhotonLarge Hadron Collider010308 nuclear & particles physicsScatteringPerturbative QCDParton7. Clean energy01 natural sciencesNuclear physicsDistribution functionPseudorapidity0103 physical sciencesHigh Energy Physics::ExperimentRapidityNuclear Experiment010306 general physicsPhysics Letters B
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Performance of the ALICE photon spectrometer PHOS

2003

Abstract We present in this paper the measured characteristics of a 64 lead–tungstate crystal array designed to detect high-energy photons and neutral mesons with the ALICE photon spectrometer PHOS. The array has been tested with electron and charged pion secondary beams delivered by the CERN PS and SPS synchrotrons. Photon energy and π 0 invariant mass resolutions are presented. The PHOS particle identification performance for data simulated with the AliRoot package is studied.

PhysicsNuclear and High Energy PhysicsPhotonLarge Hadron Collider25.75.Nq; 24.10.Lx; 25.75.-q; 29.40.VjMesonSpectrometerElectromagnetic calorimeters010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsElectronPhoton energyHigh-energy gamma rays7. Clean energy01 natural sciencesParticle identificationQuark–gluon plasmaNuclear physicsPion0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PWO scintillators010306 general physicsNuclear ExperimentInstrumentation
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A charge reconstruction algorithm for DAMPE silicon microstrip detectors

2019

Abstract The DArk Matter Particle Explorer (DAMPE) can detect electrons and photons from 5 GeV to 10 TeV and charged nuclei from a few tens of GeV to 100 TeV. The silicon–tungstentracker (STK), which is composed of 768 singled-sided silicon microstrip detectors, is one of four subdetectors in DAMPE providing photon conversion , track reconstruction, and charge identification for relativistic charged particles. This paper focuses on the charge identification performance of the STK detector. The charge response depends mainly on the incident angle and the impact position of the incoming particle. To improve the charge resolution, a reconstruction algorithm to correct for these parameters was …

PhysicsNuclear and High Energy PhysicsPhotonLarge Hadron ColliderIon beamPhysics::Instrumentation and Detectors010308 nuclear & particles physicsCharge reconstructionSTKSettore FIS/01 - Fisica SperimentaleReconstruction algorithmElectron01 natural sciencesCharged particleCharge sharingIonNuclear physicsSilicon microstrip detector0103 physical sciencesDAMPEHigh Energy Physics::ExperimentCharge sharing010303 astronomy & astrophysicsInstrumentation
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Photon emission in heavy ion collisions at the CERN SPS

2001

We compute the thermal photon spectrum in the Pb+Pb collisions at the CERN SPS energy using thermal emission rates and a hydrodynamic description for the evolution of produced hot matter and compare our results with the measurements of the excess photons by the WA98 collaboration. Our results show that the measured photon spectrum can be reproduced with realistic initial conditions which take properly into account also the finite longitudinal size of the initial collision zone and which simultaneously describe well both the transverse and longitudinal hadron spectra. In the scenario with initial formation of QGP the recently calculated emission rate, complete to order alpha_s, reproduces th…

PhysicsNuclear and High Energy PhysicsPhotonLarge Hadron ColliderNuclear TheoryHadronFOS: Physical sciencesSpectral lineNuclear Theory (nucl-th)Nuclear physicsTransverse planeHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)ThermalHeavy ionNuclear ExperimentEnergy (signal processing)
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