Search results for "Trigger"

showing 10 items of 141 documents

Overview of the high-level trigger electron and photon selection for the ATLAS experiment at the LHC

2005

texte intégral : http://cdsweb.cern.ch/record/846438; The ATLAS experiment at the Large Hadron Collider (LHC) will face the challenge of efficiently selecting interesting candidate events in$pp$collisions at 14 TeV center-of-mass energy, whilst rejecting the enormous number of background events. The High-Level Trigger (HLT$=$second level trigger and Event Filter), which is a software based trigger will need to reduce the level-1 output rate of$approx75$kHz to$approx200$Hz written out to mass storage. In this talk an overview of the current physics and system performance of the HLT selection for electrons and photons is given. The performance has been evaluated using Monte Carlo simulations …

Nuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsMonte Carlo method02 engineering and technologyElectron01 natural sciencesAtlas (anatomy)Nuclear electronics0103 physical sciences0202 electrical engineering electronic engineering information engineeringmedicine[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Electrical and Electronic EngineeringDetectors and Experimental TechniquesPhysicsLarge Hadron Collider010308 nuclear & particles physicsEvent (computing)ATLAS experiment020206 networking & telecommunicationsATLASHigh Level TriggerPhotonmedicine.anatomical_structureNuclear Energy and EngineeringFilter (video)Energy (signal processing)14th IEEE-NPSS Real Time Conference, 2005.
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The beam and detector for the NA48 neutral kaon CP violation experiment at CERN

2007

The beam and detector, used for the NA48 experiment, devoted to the measurement of Re (ε{lunate}′ / ε{lunate}), and for the NA48/1 experiment on rare KS and neutral hyperon decays, are described. © 2007 Elsevier B.V. All rights reserved.

Nuclear and High Energy PhysicsParticle physicsacceleratoriNA62 experiment01 natural sciencesLIQUID-KRYPTON CALORIMETERDECAYSNOfasci di particelleKaon beamsNuclear physicsDRIFT CHAMBER ELECTRONICSCERNViolazione di CP0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Kaon decaysdetector; CP violation; Kaon decays010306 general physicsInstrumentation07.05.Fb; 13.20.Eb; 29.40.Vj; 29.27.EgPhysicsCalorimeterLarge Hadron ColliderdetectorCRYSTAL010308 nuclear & particles physicsLIQUID-KRYPTON CALORIMETER; DRIFT CHAMBER ELECTRONICS; PROTON TAGGING DETECTOR; PC FARM; TRIGGER; SYSTEM; READOUT; DECAYS; PERFORMANCE; CRYSTALDetectorPC FARMHyperonNA48 experimentDetectorsMagnetic spectrometerPERFORMANCErivelatoriREADOUTkaon decayCalorimeterTriggerCP violationfasci di particelle; acceleratori; CERN; Violazione di CP; rivelatori; kaon decayCP violationHigh Energy Physics::ExperimentParticle Physics - ExperimentPROTON TAGGING DETECTORSYSTEMBeam (structure)
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The ATLAS level-1 trigger: Status of the system and first results from cosmic-ray data

2007

The ATLAS detector at CERN's Large Hadron Collider (LHC) will be exposed to proton-proton collisions from beams crossing at 40 MHz. At the design luminosity of 10^34 cm^-2 s^-1 there are on average 23 collisions per bunch crossing. A three-level trigger system will select potentially interesting events in order to reduce the read-out rate to about 200 Hz. The first trigger level is implemented in custom-built electronics and makes an initial fast selection based on detector data of coarse granularity. It has to reduce the rate by a factor of 10^4 to less than 100 kHz. The other two consecutive trigger levels are in software and run on PC farms. We present an overview of the first-level trig…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsAtlas detectoratlas; cosmic-ray data; installation and commissioning; trigger systemFOS: Physical sciencesCosmic rayinstallation and commissioningNuclear physicsSoftwareAtlas (anatomy)medicineatlascosmic-ray dataDetectors and Experimental TechniquesInstrumentationPhysicstrigger systemLarge Hadron ColliderLuminosity (scattering theory)business.industrySettore FIS/01 - Fisica SperimentaleDetectorInstrumentation and Detectors (physics.ins-det)medicine.anatomical_structurePhysics::Accelerator PhysicsGranularitybusinessNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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New Fast Interaction Trigger for ALICE

2017

The LHC heavy-ion luminosity and collision rate from 2021 onwards will considerably exceed the design parameters of the present ALICE forward trigger detectors and the introduction of the Muon Forward Tracker (MFT) will significantly reduce the space available for the new trigger detectors. To comply with these conditions a new Fast Interaction Trigger (FIT) will be built. FIT will be the main forward trigger, luminometer, and interaction-time detector. It will also determine multiplicity, centrality, and reaction plane of heavy-ion collisions. FIT will consist of two arrays of Cherenkov quartz radiators with MCP-PMT sensors and of a plastic scintillator ring. By increasing the overall acce…

Nuclear and High Energy PhysicsPhysics::Instrumentation and DetectorsFast Interaction TriggerScintillatorALICE upgrade01 natural sciencesPLANACON XP85012Nuclear physics0103 physical sciencesRedundancy (engineering)MCP-PMT010306 general physicsInstrumentationCherenkov radiationCollision ratePhysicsLarge Hadron ColliderMuonta114010308 nuclear & particles physicsbusiness.industryDetectorElectrical engineeringbusinessCentralityHL-LHCdetector R&DNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Fast Interaction Trigger for ALICE upgrade

2022

We present the structure, functionalities and the first in-beam performance of the ALICE Fast Interaction Trigger (FIT). FIT comprises three detectors: FT0, FV0 and FDD, which use Cherenkov and scintillation effects to detect charged particles originating from proton-proton (pp) and heavy-ion collisions. FIT generates triggers for ALICE, monitors luminosity and background, measures collision time, and determines global collision parameters, such as forward multiplicity, centrality and event plane. FIT uses dedicated front-end electronics to measure time and charge of pulses at pp bunch crossing interval of 25 ns and pp (Pb-Pb) interaction rates of up to 1 MHz (50 kHz). FIT has been installe…

Nuclear and High Energy PhysicsPhysics::Instrumentation and Detectorsdetector performanceTime resolutionhiukkasfysiikkaScintillatorALICE FIT114 Physical sciencesscintillatortrigger detectorAlice fitmittajärjestelmätDetectors and Experimental TechniquesNuclear ExperimentInstrumentationtime resolutionTrigger detectorDetector performanceCherenkov detector
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Study of BESIII trigger efficiencies with the 2018 J/psi data

2021

Using a dedicated data sample taken in 2018 on the $J/\psi$ peak, we perform a detailed study of the trigger efficiencies of the BESIII detector. The efficiencies are determined from three representative physics processes, namely Bhabha-scattering, dimuon production and generic hadronic events with charged particles. The combined efficiency of all active triggers approaches $100\%$ in most cases with uncertainties small enough as not to affect most physics analyses.

Nuclear and High Energy Physicshadronic eventsHadron01 natural sciencesNOHigh Energy Physics - ExperimentNuclear physicsSubatomär fysikBESIII; trigger efficiency; Bhabha; dimuon; hadronic events0103 physical sciencesSubatomic PhysicsBhabhaddc:530trigger efficiency010306 general physicsInstrumentationBhabha scatteringPhysicsdimuon010308 nuclear & particles physicsDetectorBESIIIAstronomy and AstrophysicsCharged particleHigh Energy Physics::ExperimentBESIII trigger efficiency Bhabha dimuon hadronic events
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Jet-like correlations with neutral pion triggers in pp and central Pb–Pb collisions at 2.76 TeV

2016

We present measurements of two-particle correlations with neutral pion trigger particles of transverse momenta 8>pT trig>16 GeV/c and associated charged particles of 0.5>pT assoc>10 GeV/c versus the azimuthal angle difference Δφ at midrapidity in pp and central Pb–Pb collisions at √sNN=2.76 TeV with ALICE. The new measurements exploit associated charged hadrons down to 0.5 GeV/c, which significantly extends our previous measurement that only used charged hadrons above 3 GeV/c. After subtracting the contributions of the flow background, v2 to v5, the per-trigger yields are extracted for |Δφ|>0.7 on the near and for |Δφ−π|>1.1 on the away side. The ratio of per-trigger yields in Pb–Pb to thos…

Nuclear and High Energy Physicsp-Pb collisionsproton-proton collisionstriggerstwo-particle correlations
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Performance of the ALICE VZERO system

2013

ALICE is an LHC experiment devoted to the study of strongly interacting matter in proton-proton, proton--nucleus and nucleus-nucleus collisions at ultra-relativistic energies. The ALICE VZERO system, made of two scintillator arrays at asymmetric positions, one on each side of the interaction point, plays a central role in ALICE. In addition to its core function as a trigger, the VZERO system is used to monitor LHC beam conditions, to reject beam-induced backgrounds and to measure basic physics quantities such as luminosity, particle multiplicity, centrality and event plane direction in nucleus-nucleus collisions. After describing the VZERO system, this publication presents its performance o…

Particle physicsPhysics::Instrumentation and DetectorsLarge detector-systems performance Trigger detectors Large detector systems for particle and astroparticle physics Heavy-ion detectorsmedia_common.quotation_subjectHeavy-ion detectorsNuclear Theorylarge detector-systems performanceFOS: Physical sciencesVZERO detectorlarge detector systems for particle and astroparticle physicsScintillator[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesAsymmetrytrigger detectors; large detector systems for particle and astroparticle physics; heavy-ion detectors; large detector-systems performancetrigger detectorsNuclear physics0103 physical sciencesALICE; trigger; V0NUCLEAR COLLISIONSNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentInstrumentationNuclear ExperimentV0 DETECTORMathematical PhysicsCore functionLarge detector-systems performance; Trigger detectors; Large detector systems for particle and astroparticle physics; Heavy-ion detectors; V0 DETECTOR; NUCLEAR COLLISIONSTrigger detectormedia_commonLarge detector-systems performancePhysicsLarge Hadron ColliderInteraction pointLarge detector systems for particle and astroparticle physics010308 nuclear & particles physicsALICE experimentTrigger detectorsLarge detector systems for particle and astroparticle physicheavy-ion detectorsComputingMethodologies_DOCUMENTANDTEXTPROCESSINGCentralityLarge detector-systems performance; Trigger detectors; Large detector systems for particle and astroparticle physics; Heavy-ion detectorsParticle Physics - Experiment
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Functional Magnetic Mesoporous Silica Microparticles Capped with an Azo-Derivative: A Promising Colon Drug Delivery Device

2018

[EN] Magnetic micro-sized mesoporous silica particles were used for the preparation of a gated material able to release an entrapped cargo in the presence of an azo-reducing agent and, to some extent, at acidic pH. The magnetic mesoporous microparticles were loaded with safranin O and the external surface was functionalized with an azo derivative 1 (bearing a carbamate linkage) yielding solid S1. Aqueous suspensions of S1 at pH 7.4 showed negligible safranin O release due to the presence of the bulky azo derivative attached onto the external surface of the inorganic scaffold. However, in the presence of sodium dithionite (azoreductive agent), a remarkable safranin O delivery was observed. A…

Pharmaceutical Science02 engineering and technologyFerric Compounds01 natural sciencesazo reductorcolon releaseAnalytical ChemistrySodium dithionitechemistry.chemical_compoundQUIMICA ORGANICADrug DiscoveryMoietymagnetic mesoporous silicaDrug CarriersAqueous solutionHydrolysisHydrogen-Ion ConcentrationSilicon Dioxide021001 nanoscience & nanotechnologyControlled releaseMicrospheresChemistry (miscellaneous)Drug deliveryMolecular Medicine0210 nano-technologyOxidation-ReductionPorosityColonSurface Properties010402 general chemistryArticleMagneticsChloridesSafraninQUIMICA ANALITICAHumansFerrous CompoundsPhysical and Theoretical Chemistrymagnetic mesoporous silica; azo derivatives; pH triggered; azo reductor; colon releaseQUIMICA INORGANICAOrganic ChemistryDithioniteMesoporous silica0104 chemical sciencesDrug LiberationchemistryNanoparticlesPhenazinespH triggeredMesoporous materialAzo Compoundsazo derivativesNuclear chemistryMolecules; Volume 23; Issue 2; Pages: 375
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Time of flight measurements based on FPGA using a breast dedicated PET

2014

In this work the implementation of a Time-to-Digital Converter (TDC) using a Nutt delay line FPGA-based and applied on a Positron Emission Tomography (PET) device is going to be presented in order to check the system’s suitability for Time of Flight (TOF) measurements. In recent years, FPGAs have shown great advantages for precise time measurements in PET. The architecture employed for these measurements is described in detail. The system developed was tested on a dedicated breast PET prototype, composed of LYSO crystals and Positive Sensitive Photomultipliers (PSPMTs). Two distinct experiments were carried out for this purpose. In the first test, system linearity was evaluated in order to …

PhotomultiplierImage qualityComputer scienceInstrumentation and methods for time-of-flight (TOF) spectroscopyLinearityTrigger detectorsCoincidenceLyso-Time of flightLine (geometry)TEORIA DE LA SEÑAL Y COMUNICACIONESField-programmable gate arrayInstrumentationMathematical PhysicsSimulation
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