Search results for " Collider"

showing 10 items of 1415 documents

Comparison of Fragmentation Functions for Jets Dominated by Light Quarks and Gluons from pp and Pb+Pb Collisions in ATLAS

2019

Charged-particle fragmentation functions for jets azimuthally balanced by a high-transverse-momentum, prompt, isolated photon are measured in 25  pb^{-1} of pp and 0.49  nb^{-1} of Pb+Pb collision data at 5.02 TeV per nucleon pair recorded with the ATLAS detector at the Large Hadron Collider. The measurements are compared to predictions of Monte Carlo generators and to measurements of inclusively selected jets. In pp collisions, a different jet fragmentation function in photon-tagged events from that in inclusive jet events arises from the difference in fragmentation between light quarks and gluons. The ratios of the fragmentation functions in Pb+Pb events to that in pp events are used to e…

PhysicsLarge Hadron ColliderPhotonAstrophysics::High Energy Astrophysical PhenomenaGeneral Physics and AstronomyParton01 natural sciencesCharged particleNuclear physicsFragmentation (mass spectrometry)0103 physical sciencesQuark–gluon plasmaHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNucleonJet quenchingPhysical Review Letters
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Probing nuclear PDFs with dijets in ultra-peripheral Pb+Pb collisions

2019

In this talk we apply the photoproduction framework recently implemented into the Pythia 8 Monte Carlo event generator to study the potential of photo-nuclear dijets in ultra-peripheral Pb+Pb collisions at the LHC to further constrain the nuclear PDFs. These events can be described as $\gamma$A collisions where the relevant part of the flux of quasi-real photons from heavy-ions is obtained by using the equivalent photon approximation and cutting out impact-parameter values which would lead to hadronic interactions between the beam particles. In particular, we quantify the small-$x$ reach with different jet kinematics and show how well the values of $x$ derived from reconstructed jet momenta…

PhysicsLarge Hadron ColliderPhotonHadronMonte Carlo methodFOS: Physical sciencesFluxhiukkasfysiikkaJet (particle physics)Nuclear physicsMomentumHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)ydinfysiikkaNuclear ExperimentEvent generatorProceedings of International Conference on Hard and Electromagnetic Probes of High-Energy Nuclear Collisions — PoS(HardProbes2018)
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Medium-Induced Modification of Z -Tagged Charged Particle Yields in Pb+Pb Collisions at 5.02 TeV with the ATLAS Detector

2021

The yield of charged particles opposite to a Z boson with large transverse momentum (p_{T}) is measured in 260  pb^{-1} of pp and 1.7  nb^{-1} of Pb+Pb collision data at 5.02 TeV per nucleon pair recorded with the ATLAS detector at the Large Hadron Collider. The Z boson tag is used to select hard-scattered partons with specific kinematics, and to observe how their showers are modified as they propagate through the quark-gluon plasma created in Pb+Pb collisions. Compared with pp collisions, charged-particle yields in Pb+Pb collisions show significant modifications as a function of charged-particle p_{T} in a way that depends on event centrality and Z boson p_{T}. The data are compared with a…

PhysicsLarge Hadron ColliderPhotonHigh Energy Physics::PhenomenologyGeneral Physics and AstronomyParton7. Clean energy01 natural sciencesCharged particleNuclear physicsmedicine.anatomical_structureAtlas (anatomy)0103 physical sciencesQuark–gluon plasmamedicineHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsNucleonBosonPhysical Review Letters
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Search for polarization effects in the antiproton production process

2015

For the production of a polarized antiproton beam various methods have been suggested including the possibility that antiprotons may be produced polarized which will be checked experimentally. The polarization of antiprotons produced under typical conditions for antiproton beam preparation will be measured at the CERN/PS. If the production process creates some polarization a polarized antiproton beam could be prepared by a rather simple modification of the antiproton beam facility. The detection setup and the expected experimental conditions are described. For the production of a polarized antiproton beam various methods have been suggested including the possibility that antiprotons may be …

PhysicsLarge Hadron ColliderPhysics - Instrumentation and DetectorsFOS: Physical sciencesGeneral Physics and AstronomyParticle acceleratorInstrumentation and Detectors (physics.ins-det)Polarization (waves)law.inventionHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)Antiproton beamAntiprotonlawPhysics::Accelerator Physicsddc:530High Energy Physics::ExperimentPhysics::Atomic PhysicsNuclear Experiment (nucl-ex)Detectors and Experimental TechniquesNuclear ExperimentNuclear Experiment
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Production ofD, D * andD s mesons in 200 GeV/c ?? K ? andp-Si interactions

1988

The NA 32 experiment at the CERN SPS has collected 38 million hadronic interactions with incident 200 GeV/c π−,K− andp beam. Using a segmented silicon active target and a telescope of high resolution silicon microstrip counters we have selected fully reconstructedD0→K−π+,D0→K−π+π+π−,D+→K−π+π+,Ds+→K−K+π+π+ and charge conjugate decays. The integrated cross-sections forDo,D+D*+ andDs+ meson production and the dependence of the cross-section on longitudinal and transverse momentum of theD are presented.

PhysicsLarge Hadron ColliderPhysics and Astronomy (miscellaneous)SiliconMesonHadronchemistry.chemical_elementCharge (physics)Elementary particleNuclear physicschemistryEngineering (miscellaneous)Particle Physics - ExperimentBeam (structure)ConjugateZeitschrift f�r Physik C Particles and Fields
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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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Search for long-lived neutral particles produced in pp collisions at s=13  TeV decaying into displaced hadronic jets in the ATLAS inner detector and …

2020

A search is presented for pair production of long-lived neutral particles using 33     fb − 1 of √ s = 13     TeV proton–proton collision data, collected during 2016 by the ATLAS detector at the LHC. This search focuses on a topology in which one long-lived particle decays in the ATLAS inner detector and the other decays in the muon spectrometer. Special techniques are employed to reconstruct the displaced tracks and vertices in the inner detector and in the muon spectrometer. One event is observed that passes the full event selection, which is consistent with the estimated background. Limits are placed on scalar boson propagators with masses from 125 GeV to 1000 GeV decaying into pairs of …

PhysicsLarge Hadron ColliderPhysics::Instrumentation and Detectors010308 nuclear & particles physicsAtlas (topology)HadronDetectorPropagatorScalar boson01 natural sciencesNuclear physicsHidden sectorPair production0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsPhysical Review D
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The Topological Processor for the future ATLAS Level-1 Trigger: From design to commissioning

2014

The ATLAS detector at the Large Hadron Collider (LHC) is designed to measure decay properties of high energetic particles produced in the proton-proton collisions. During its first run, the LHC collided proton bunches at a frequency of 20 MHz, and therefore the detector required a Trigger system to efficiently select events down to a manageable event storage rate of about 400 Hz. By 2015 the LHC instantaneous luminosity will be increased up to 3×1034cm−2s−1: this represents an unprecedented challenge faced by the ATLAS Trigger system. To cope with the higher event rate and efficiently select relevant events from a physics point of view, a new element will be included in the Level-1 Trigger …

PhysicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsEvent (computing)VHDLDetectorSignal integrityLatency (engineering)TopologyField-programmable gate arraycomputercomputer.programming_languageData transmission2014 19th IEEE-NPSS Real Time Conference
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An FPGA based demonstrator for a topological processor in the future ATLAS L1-Calo trigger “GOLD”

2012

Abstract: The existing ATLAS trigger consists of three levels. The level 1 (L1) is an FPGAs based custom designed trigger, while the second and third levels are software based. The LHC machine plans to bring the beam energy to the maximum value of 7 TeV and to increase the luminosity in the coming years. The current L1 trigger system is therefore seriously challenged. To cope with the resulting higher event rate, as part of the ATLAS trigger upgrade, a new electronics module is foreseen to be added in the ATLAS Level-1 Calorimeter Trigger electronics chain: the Topological Processor (TP). Such a processor needs fast optical I/O and large aggregate bandwidth to use the information on trigger…

PhysicsLarge Hadron ColliderPhysics::Instrumentation and Detectorsbusiness.industryBandwidth (signal processing)TopologyCalorimeterSoftwareUpgradeHigh Energy Physics::ExperimentElectronicsDetectors and Experimental TechniquesbusinessField-programmable gate arrayInstrumentationMathematical PhysicsElectronic circuitJournal of Instrumentation
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First Capture of Antiprotons in an Ion Trap: Progress Toward a Precision Mass Measurement and Antihydrogen

1988

Antiprotons from the Low Energy Antiproton Ring of CERN are slowed from 21 MeV to below 3 keV by being passed through 3 mm of material, mostly Be. While still in flight, the kilo-electron volt antiprotons are captured in a Penning trap created by the sudden application of a 3-kV potential. Antiprotons are held for 100 s and more. Prospects are now excellent for much longer trapping times under better vacuum conditions. This demonstrates the feasibility of a greatly improved measurement of the inertial mass of the antiproton and opens the way to other intriguing experiments. The possibility of producing antihydrogen by merging cold, trapped plasmas of positrons and antiprotons is discussed.

PhysicsLarge Hadron ColliderPlasmaCondensed Matter PhysicsPenning trapMass measurementAtomic and Molecular Physics and OpticsNuclear physicsAntiprotonPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentPhysics::Atomic PhysicsIon trapInertial massNuclear ExperimentAntihydrogenMathematical PhysicsPhysica Scripta
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