Search results for "Experimental techniques"

showing 10 items of 226 documents

DEPFET Active Pixel Detectors for a Future Linear e(+)e(-) Collider

2013

arXiv:1212.2160v1.-- et al.

Vertex (graph theory)Nuclear and High Energy PhysicsParticle physicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and Detectorsvertex detectorComputingMethodologies_IMAGEPROCESSINGANDCOMPUTERVISIONFOS: Physical sciences01 natural sciencesHigh Energy Physics - Experimentlaw.inventionHigh Energy Physics - Experiment (hep-ex)Signal-to-noise ratiolaw0103 physical sciencesElectrical and Electronic EngineeringDetectors and Experimental Techniques010306 general physicsColliderPrecision Pixel Detectors [9.3]ComputingMethodologies_COMPUTERGRAPHICSAdvanced infrastructures for detector R&D [9]PhysicsPixel010308 nuclear & particles physicsDetectorFísicaInstrumentation and Detectors (physics.ins-det)Active pixel sensorNuclear Energy and EngineeringHigh Energy Physics::ExperimentVertex detectorlinear colliderddc:620DEPFETPixel detector
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ATLAS Inner Detector alignment and analysis of the Wtb vertex structure with single top quarks

2018

Esta tesis puede ser dividida en dos partes diferentes: La primera trata sobre el alineamiento del detector interno de ATLAS, y la segunda sobre el estudio de la estructura del vértice Wtb mediante el uso de quarks top producidos en solitario. La primera parte presenta las técnicas utilizadas para alinear el detector interno de ATLAS, así como las mejoras implementadas en algoritmo de alineamiento durante el Run-II del LHC. Durante la toma de datos, tienen lugar en el detector interno diversos movimientos y deformaciones dinámicos que comprometen la calidad de los datos recogidos. Los dos más relevantes son un movimiento vertical del detector de Píxeles, y el combado del IBL. En el alineami…

anomalous couplingsweak interaction221502 - Física experimental de altas energíasalignment221500 - Física de altas energíasHigh Energy Physics::ExperimentATLASDetectors and Experimental TechniquesInner Detectortop quarksingle top220807 - Física de partículas
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Real-time data processing in the ALICE High Level Trigger at the LHC

2019

At the Large Hadron Collider at CERN in Geneva, Switzerland, atomic nuclei are collided at ultra-relativistic energies. Many final-state particles are produced in each collision and their properties are measured by the ALICE detector. The detector signals induced by the produced particles are digitized leading to data rates that are in excess of 48 GB/$s$. The ALICE High Level Trigger (HLT) system pioneered the use of FPGA- and GPU-based algorithms to reconstruct charged-particle trajectories and reduce the data size in real time. The results of the reconstruction of the collision events, available online, are used for high level data quality and detector-performance monitoring and real-tim…

calibration ; ALICE ; trigger ; monitoring ; quality ; data management ; programming ; FPGA ; multiprocessor: graphics ; performancePhysics - Instrumentation and DetectorsHigh level triggerPhysics::Instrumentation and DetectorsLevel datatutkimuslaitteetFPGA; GPUDetector calibrationGPUFOS: Physical sciencesGeneral Physics and AstronomyhiukkasfysiikkaPhysics and Astronomy(all)01 natural sciencesprogramming010305 fluids & plasmasCombinatoricsALICE0103 physical sciencesmultiprocessor: graphics[INFO]Computer Science [cs][PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental Techniques010306 general physicsNuclear Experimentphysics.ins-detFPGAcomputer.programming_languagePhysicsLarge Hadron ColliderFPGA; GPU; TRACKsignaalinkäsittelyInstrumentation and Detectors (physics.ins-det)triggercalibrationmonitoringdatailmaisimetqualityHardware and ArchitectureTRACKHigh Energy Physics::Experimentdata managementAlice (programming language)computerperformance
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Performance of $b$-Jet Identification in the ATLAS Experiment

2016

We thank CERN for the very successful operation of the LHC, as well as the support staff from our institutions without whom ATLAS could not be operated efficiently. We acknowledge the support of ANPCyT, Argentina; YerPhI, Armenia; ARC, Australia; BMWFW and FWF, Austria; ANAS, Azerbaijan; SSTC, Belarus; CNPq and FAPESP, Brazil; NSERC, NRC and CFI, Canada; CERN; CONICYT, Chile; CAS, MOST and NSFC, China; COLCIENCIAS, Colombia; MSMT CR, MPO CR and VSC CR, Czech Republic; DNRF, DNSRC and Lundbeck Foundation, Denmark; IN2P3-CNRS, CEA-DSM/IRFU, France; GNSF, Georgia; BMBF, HGF, and MPG, Germany; GSRT, Greece; RGC, Hong Kong SAR, China; ISF, I-CORE and Benoziyo Center, Israel; INFN, Italy; MEXT an…

detector-systems performancePerformance of High Energy Physics Detectorsecondary [vertex]Elementary particle01 natural sciencesPARTONlaw.inventionSubatomär fysikCHANNELcluster findingscattering [p p]impact parameterGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)протон-протонные столкновенияQBLarge detector-systems performanceHigh energy physics detectorLarge Hadron ColliderLarge detector systems for particle and astroparticle physics; Large detector-systems performance; Pattern recognition cluster finding calibration and fitting methods; Performance of High Energy Physics Detectors; Instrumentation; Mathematical Physicstrack data analysisQUARK PAIR PRODUCTIONbottom [jet]CERN LHC CollPattern recognition cluster finding calibration and fitting method7000 GeV-cmscolliding beams [p p]performanceHADRONIC COLLISIONSCiências Naturais::Ciências FísicasLarge detectorFitting methodHigh energy physicATLAS LHC High Energy Physics510 MathematicsmuonDISTRIBUTIONSUncertainty analysis Astroparticle physicHigh Energy Physics010306 general physicsSystematic uncertainties AlgorithmsAstroparticle physicsCalibration and fitting methodsScience & Technology010308 nuclear & particles physicsLarge detector systems for particle and astroparticle physicsParticle acceleratorRangingPerformance of High Energy PhysicsCOLLIDERScorrelationExperimental High Energy PhysicsPerformance of High Energy Physics DetectorshadronATLAS детекторБольшой адронный коллайдерcharm [jet]Elementary particleHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)lawSubatomic Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Detectors and Experimental TechniquesInstrumentationUncertainty analysisMathematical PhysicsPhysicsPattern recognition cluster finding calibration and fitting methods4. EducationATLAS experimentSettore FIS/01 - Fisica SperimentaleDetectorsflavor [jet]calibration and fitting methodsATLASLarge Hadron ColliderLarge detector systems for particle and astroparticle physics; Large; detector-systems performance; Pattern recognition cluster finding; calibration and fitting methods; Performance of High Energy Physics; Detectors; PRODUCTION CROSS-SECTION; QUARK PAIR PRODUCTION; ROOT-S=7 TEV; PARTON; DISTRIBUTIONS; HADRONIC COLLISIONS; MATRIX-ELEMENTS; LHC; COLLIDERS; DETECTOR; CHANNEL8. Economic growthCalibrationparticle identification [bottom]LHCImpact parameterParticle Physics - ExperimentParticle physicsdata analysis method530 Physics:Ciências Físicas [Ciências Naturais]FOS: Physical sciences530MATRIX-ELEMENTSparticle identification [charm]on-line [trigger]Pattern recognition0103 physical sciencesComplementary methodddc:610DETECTORROOT-S=7 TEVCluster findingFísicaLarge detector systems for particle and astroparticle physics; Large detector-systems performance; Pattern recognition cluster finding calibration and fitting methods; Performance of High Energy Physics DetectorsPattern recognition systemcalibrationtracksPRODUCTION CROSS-SECTIONefficiencyHadronLarge detector systems for particle and astroparticle physicLargeHigh Energy Physics::ExperimentStatistical correlationstatisticalexperimental results
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Measurement of the SMC muon beam polarisation using the asymmetry in the elastic scattering off polarised electrons

2000

A muon beam polarimeter was built for the SMC experiment at the CERN SPS, for beam energies of 100 and 190 GeV. The beam polarisation is determined from the asymmetry in the elastic scattering off the polarised electrons of a ferromagnetic target whose magnetisation is periodically reversed. At muon energies of 100 and 190 GeV the measured polarisation is P-mu = -0.80 +/- 0.03 (stat.) +/- 0.02 (syst.) and P-mu = - 0.797 +/- 0.011 (stat.) +/- 0.012 (syst.), respectively. These results agree with measurements of the beam polarisation using a shape analysis of the decay positron energy spectrum. (C) 2000 Elsevier Science B.V. All rights reserved.

electronNuclear and High Energy PhysicsSMC; DIS; muon polarimetermedia_common.quotation_subjectmuon beamElectronAsymmetryNuclear physicsMagnetizationpolarisation measurementDetectors and Experimental TechniquesNuclear ExperimentInstrumentationmedia_commonPhysicsElastic scatteringDISLarge Hadron ColliderMuonpolarised scatteringSMCmagnetised targetPolarimeterpolarised muonPolarization (waves)muon polarimeterPhysics::Accelerator PhysicsHigh Energy Physics::Experimentpolarised
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Detection of charged kaons using the decay topology in ALICE TPC

2006

hiukkasetkaonitDetectors and Experimental TechniquesfysiikkaydintutkimusParticle Physics - Experiment
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Silicon Strip Detectors for the ATLAS End-Cap Tracker at the HL-LHC

2017

El LHC se ha convertido en el acelerador más potente de todos los tiempos. Su principal objetivo es dar respuesta a las limitaciones del Modelo Estándar y revelar la física más allá de él. El descubrimiento del bosón de Higgs en 2012 supuso el comienzo de una era en el campo de la física de partículas donde conseguir la mayor precisión posible en las medidas es vital. En el LHC se aceleran y colisionan protones con una energía nominal de centro de masas de 14 TeV y una luminosidad instantánea nominal de 10^34 cm−2 s−1. Para la máxima luminosidad, los protones son acelerados en paquetes de 1.15 ×10^11 protones cada uno, con una frecuencia de 40 MHz (esto supone una colisión cada 25 ns). Esta…

hl-lhcdetectoressilicioPhysics::Instrumentation and Detectors:FÍSICA [UNESCO]radiaciónUNESCO::FÍSICAaceleradoresDetectors and Experimental Techniqueslhc
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Design and development of safety and control systems in ATLAS

2021

El gran colisionador de hadrones, o LHC, es el acelerador de partículas más grande y potente del mundo. Ha sido construido por el CERN, la Organización Europea para la Investigación Nuclear, entre 1998 y 2008 en Ginebra, Suiza. Sucesivas mejoras en el LHC supondrán a partir de mediados del 2027 un incremento de la luminosidad, cuando pasará a llamarse High Luminosity LHC (HL-LHC). Esta tesis se divide en dos partes, por una parte la seguridad y operación de la infraestructura y por otra los sistemas de control y toma de datos. La primera parte de la tesis se dedica a la seguridad y operación de la infraestructura. Después de más de 10 años de funcionamiento, el riesgo de posibles fallos en …

leak detectionhadiation hardness:CIENCIAS TECNOLÓGICAS [UNESCO]CMOSexpert systemsLHCDetectors and Experimental TechniquesATLASUNESCO::CIENCIAS TECNOLÓGICASbeam telescopeSEU
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Latest Developments and Results of Radiation Tolerance CMOS Sensors with Small Collection Electrodes

2020

The development of radiation hard Depleted Monolithic Active Pixel Sensors (DMAPS) targets the replacement of hybrid pixel detectors to meet radiation hardness requirements of at least 1.5e16 1 MeV neq/cm2 for the HL-LHC and beyond. DMAPS were designed and tested in the TJ180 nm TowerJazz CMOS imaging technology with small electrodes pixel designs. This technology reduces costs and provides granularity of 36.4x36.4 um2 with low power operation (1 uW/pixel), low noise of ENC < 20 e-, a small collection electrode (3 um) and fast signal response within 25 ns bunch crossing. This contribution will present the latest developments after the MALTA and Mini-MALTA sensors. It will illustrate the imp…

noiseParticle tracking detectors ; Radiation-hard detectors ; Electronic detector readout concepts ; CMOS sensors ; Monolithic active pixel sensorsMaterials science010308 nuclear & particles physicsbusiness.industryintegrated circuitelectrode01 natural sciencesCMOSRadiation toleranceefficiency0103 physical sciencesElectrodeHardware_INTEGRATEDCIRCUITSelectronics: readoutOptoelectronicssemiconductor detector[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental Techniquescontrol system010306 general physicsbusiness
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Study of scintillation light collection, production and propagation in a 4 tonne dual-phase LArTPC

2020

The $3 \times 1 \times 1$ m$^3$ demonstrator is a dual phase liquid argon time projection chamber that has recorded cosmic rays events in 2017 at CERN. The light signal in these detectors is crucial to provide precise timing capabilities. The performances of the photon detection system, composed of five PMTs, are discussed. The collected scintillation and electroluminescence light created by passing particles has been studied in various detector conditions. In particular, the scintillation light production and propagation processes have been analyzed and compared to simulations, improving the understanding of some liquid argon properties.

photon: propagationPhotomultiplierCERN LabPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorstutkimuslaitteetPerformance of High Energy Physics DetectorPhase (waves)FOS: Physical sciencesCosmic rayNoble liquid detectors (scintillation ionization double-phase)Scintillator01 natural sciences7. Clean energyHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)Optics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex][PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental Techniques010306 general physicsInstrumentationphysics.ins-detMathematical Physicsscintillation counterPhysicsScintillationTime projection chamberphotomultiplier010308 nuclear & particles physicsbusiness.industryhep-exDetectorScintillators scintillation and light emission processes (solid gas and liquid scintillators)Instrumentation and Detectors (physics.ins-det)time projection chamber: liquid argonNoble liquid detectors (scintillation ionization double-phase); Performance of High Energy Physics Detectors; Photon detectors for UV visible and IR photons (vacuum) (photomulti-pliers HPDs others); Scintillators scintillation and light emission processes (solid gas and liquidscintillators)Photon detectors for UV visible and IR photons (vacuum) (photomultipliers HPDs others)FIS/01 - FISICA SPERIMENTALEilmaisimetScintillation counterbusinesskosminen säteilyperformanceParticle Physics - Experiment
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