0000000000520765

AUTHOR

A. Falou

showing 2 related works from this author

Beam test results of IHEP-NDL Low Gain Avalanche Detectors(LGAD)

2020

A High-Granularity Timing Detector (HGTD) is proposed based on the Low-Gain Avalanche Detector (LGAD) for the ATLAS experiment to satisfy the time resolution requirement for the up-coming High Luminosity at LHC (HL-LHC). We report on beam test results for two proto-types LGADs (BV60 and BV170) developed for the HGTD. Such modules were manufactured by the Institute of High Energy Physics (IHEP) of Chinese Academy of Sciences (CAS) collaborated with Novel Device Laboratory (NDL) of the Beijing Normal University. The beam tests were performed with 5 GeV electron beam at DESY. The timing performance of the LGADs was compared to a trigger counter consisting of a quartz bar coupled to a SiPM read…

Electron beamNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsFÍSICA DE ALTA ENERGIAPhysics::Instrumentation and DetectorsFOS: Physical sciences01 natural sciences010305 fluids & plasmassymbols.namesakeSilicon photomultiplierOpticsLGAD0103 physical sciencesGaussian functionelectron: irradiationphotomultiplier: silicon[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental Techniques010306 general physicsInstrumentationphysics.ins-detPhysicsLarge Hadron ColliderLuminosity (scattering theory)business.industryfluctuationDetectorATLAS experimentTime resolutionDESYInstrumentation and Detectors (physics.ins-det)ATLASsymbolsHigh Energy Physics::ExperimentbusinessCFDBeam (structure)performancesemiconductor detector: design
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Beam test measurements of Low Gain Avalanche Detector single pads and arrays for the ATLAS High Granularity Timing Detector

2018

For the high luminosity upgrade of the LHC at CERN, ATLAS is considering the addition of a High Granularity Timing Detector (HGTD) in front of the end cap and forward calorimeters at |z|= 3.5 m and covering the region 2.4 <|η|< 4 to help reducing the effect of pile-up. The chosen sensors are arrays of 50 μm thin Low Gain Avalanche Detectors (LGAD). This paper presents results on single LGAD sensors with a surface area of 1.3×1.3 mm2 and arrays with 2×2 pads with a surface area of 2×2 mm2 or 3×3 mm2 each and different implant doses of the p+ multiplication layer. They are obtained from data collected during a beam test campaign in autumn 2016 with a pion beam of 120 GeV energy at the CERN SP…

Physics - Instrumentation and DetectorsPhysics::Instrumentation and Detectorsionization: yieldFOS: Physical sciences01 natural sciencesTiming detectorsParticle detectorHigh Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)OpticsAtlas (anatomy)0103 physical sciencesmedicine[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Detectors and Experimental TechniquesSolid state detectors010306 general physicsphysics.ins-det[ PHYS.PHYS.PHYS-INS-DET ] Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]Instrumentationspatial resolutiontime resolutionMathematical PhysicsPhysicsLarge Hadron ColliderLuminosity (scattering theory)010308 nuclear & particles physicsbusiness.industryHigh Energy Physics::PhenomenologyDetectorInstrumentation and Detectors (physics.ins-det)ATLASSi microstrip and pad detectorsSemiconductor detectormedicine.anatomical_structurepile-upavalancheefficiencyPhysics::Accelerator Physicssemiconductor detectorHigh Energy Physics::ExperimentGranularitybusinessBeam (structure)
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