Search results for "racking"

showing 10 items of 815 documents

Interaction position resolution simulations and in-beam measurements of the AGATA HPGe detectors

2011

WOS: 000290082600015

Nuclear and High Energy PhysicsFusion-evaporation ReactionsPhysics::Instrumentation and Detectorsg-ray trackingAstrophysics::High Energy Astrophysical PhenomenaMonte Carlo methodEvaporationRay tracking[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesParticle detectorNuclear physicsAGATA Fusion-evaporation reactions HPGe detectors Monte Carlo Simulation Ray tracking; Computer simulation Evaporation Monte Carlo methods Phase transitions; DetectorsHPGe Detectors0103 physical sciencesNuclear Experiment010306 general physicsInstrumentationGamma-ray TrackingPhysics010308 nuclear & particles physics4. EducationResolution (electron density)DetectorMonte Carlo SimulationMonte Carlo methodsDetectorsComputer simulationSemiconductor detectorPhase transitionsMonte Carlo SimulationsMeasuring instrumentHigh Energy Physics::ExperimentAGATAAGATABeam (structure)
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Pairing-quadrupole interplay in the neutron-deficient tin nuclei: First lifetime measurements of low-lying states in 106,108Sn

2020

The lifetimes of the low-lying excited states 2(+) and 4(+) have been directly measured in the neutron-deficient Sn-106,Sn-108 isotopes. the nuclei were populated via a deep-inelastic reaction and the lifetime measurement was performed employing a differential plunger device. the emitted gamma rays were detected by the AGATA array, while the reaction products were uniquely identified by the VAMOS++ magnetic spectrometer. Large-Scale Shell-Model calculations with realistic forces indicate that, independently of the pairing content of the interaction, the quadrupole force is dominant in the B(E2; 2(1)(+) -> 0(g.s)(+)) values and it describes well the experimental pattern for Sn104-114 ; the B…

Nuclear and High Energy PhysicsLight Snchemistry.chemical_elementFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]nucl-ex01 natural sciencesSubatomär fysikLifetime; Light Sn; Multi-nucleon transfer; Nuclear structure; Tracking array0103 physical sciencesSubatomic PhysicsNeutronTracking arrayNuclear Physics - ExperimentNuclear structureNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentPhysicsSpectrometerIsotopeLifetime ; Nuclear structure ; Multi-nucleon transfer ; Light Sn ; Tracking array010308 nuclear & particles physicsPhysicsMulti-nucleon transferlcsh:QC1-999chemistryPairingExcited stateQuadrupoleAGATAAtomic physicsTinlcsh:PhysicsLifetime
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Tracking with heavily irradiated silicon detectors operated at cryogenic temperatures

1998

In this work we show that a heavily irradiated double-sided silicon microstrip detector recovers its performance when operated at cryogenic temperatures. A DELPHI microstrip detector, irradiated to a fluence of /spl sim/4/spl times/10/sup 14/ p/cm/sup 2/, no longer operational at room temperature, cannot be distinguished from a non-irradiated one when operated at T<120 K. Besides confirming the previously observed 'Lazarus effect' in single diodes, these results establish, for the first time, the possibility of using standard silicon detectors for tracking applications in extremely demanding radiation environments.

Nuclear and High Energy PhysicsMaterials sciencePassivationSiliconbusiness.industryDetectorchemistry.chemical_elementRadiationTracking (particle physics)FluenceNuclear Energy and EngineeringchemistryOptoelectronicsIrradiationDetectors and Experimental TechniquesElectrical and Electronic EngineeringbusinessDiodeIEEE Transactions on Nuclear Science
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Time projection chambers for the T2K near detectors

2011

The T2K experiment is designed to study neutrino oscillation properties by directing a high intensity neutrino beam produced at J-PARC in Tokai, Japan, towards the large Super-Kamiokande detector located 295 km away, in Kamioka, Japan. The experiment includes a sophisticated near detector complex, 280 m downstream of the neutrino production target in order to measure the properties of the neutrino beam and to better understand neutrino interactions at the energy scale below a few GeV. A key element of the near detectors is the ND280 tracker, consisting of two active scintillator–bar target systems surrounded by three large time projection chambers (TPCs) for charged particle tracking. The d…

Nuclear and High Energy PhysicsNeutrino oscillationPhysics::Instrumentation and Detectorsddc:500.2Tracking (particle physics)01 natural sciences7. Clean energyNuclear physics0103 physical sciences010306 general physicsNeutrino oscillationInstrumentationPhysicsTime projection chamber010308 nuclear & particles physicsDetectorT2K experimentDrift chamber Gas system Micromegas Neutrino oscillation Time projection chamberFísicaMicroMegas detectorTime projectionchamberGas systemCharged particleTime projection chamberDrift chamberHigh Energy Physics::ExperimentNeutrinoMicromegas
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Design of large scale sensors in 180 nm CMOS process modified for radiation tolerance

2019

International audience; The last couple of years have seen the development of Depleted Monolithic Active Pixel Sensors (DMAPS) fabricated with a process modification to increase the radiation tolerance. Two large scale prototypes, Monopix with a column drain synchronous readout, and MALTA with a novel asynchronous architecture, have been fully tested and characterized both in the laboratory and in test beams. This showed that certain aspects have to be improved such as charge collection after irradiation and the output data rate. Some improvements resulting from extensive TCAD simulations were verified on a small test chip, Mini-MALTA. A detailed cluster analysis, using data from laboratory…

Nuclear and High Energy PhysicsOn-chip clusteringPhysics::Instrumentation and Detectors01 natural sciencesCMOS sensors ; Tracking detectors ; Monolithic sensors ; MAPS ; On-chip clustering030218 nuclear medicine & medical imaging03 medical and health sciencesTracking detectors0302 clinical medicinesemiconductor detector: pixelRadiation toleranceCMOS sensors0103 physical sciencesMAPSElectronic engineeringIrradiation[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]numerical calculationsInstrumentationradiation: damagePhysicsPixelirradiation010308 nuclear & particles physicstracking detector: upgradecharge: yieldBandwidth (signal processing)ATLASDigital architectureChipUpgradeAsynchronous communicationMonolithic sensors
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Search for particles with unexpected mass and charge in Z decays

1993

During 1989 and 1990 over 180 000 hadronic and leptonic events, corresponding to 8 pb-1 of luminosity, were collected by the ALEPH detector in a scan of the Z peak at the e+e- collider LEP. This letter reports the results of a search in these data for particles with unexpected mass and charge by measurement of the ionization energy loss of charged tracks in the ALEPH TPC central tracking detector. The mass limits for the pair production of fractionally charged particles and of heavy, long lived charged particles are extended to 43 GeV/c2 at 90% confidence level. If single production of a heavy particle is considered, the mass limit is extended to more than 70 GeV/c2. RI Perrier, Frederic/A-…

Nuclear and High Energy PhysicsParticle physicsAlephElectron–positron annihilationHadronTracking (particle physics)01 natural scienceslaw.inventionALEPH ExperimentNuclear physicslaw0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment010306 general physicsColliderPhysicsLuminosity (scattering theory)010308 nuclear & particles physicsPhysicslcsh:QC1-999Charged particlePair productionHigh Energy Physics::Experimentlcsh:PhysicsParticle Physics - Experiment
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Search for exclusive decays of the Lambda_b baryon and measurement of its mass

1996

A search for fully reconstructed \lb beauty baryons is performed using about 3 million Z decays collected with the DELPHI detector at LEP. The analysis relies on the combined use of the accurate tracking and of the hadron identification capabilities of DELPHI. A total of four events has been found, three in the \lc\ppm channel and one in the \lc\a1m channel over a small background. The \lb beauty baryon mass is measured to be (~ 5668 \pm 16~ ({\rm stat.}) \pm 8~({\rm syst.})~)~ \mv.

Nuclear and High Energy PhysicsParticle physicsHadronCombined useLambdaTracking (particle physics)01 natural sciencesPartícules (Física nuclear)Nuclear physicsbeauty baryon0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]010306 general physicsNuclear ExperimentDetectors de radiacióDELPHIPhysics010308 nuclear & particles physicsDetectorLARGE ELECTRON POSITRON COLLIDERBaryonDELPHI; beauty baryon; particle identificationPARTICLE PHYSICS; LARGE ELECTRON POSITRON COLLIDER; DELPHIPARTICLE PHYSICSHigh Energy Physics::Experimentparticle identificationParticle Physics - Experiment
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Technical design of the phase I Mu3e experiment

2021

Nuclear instruments &amp; methods in physics research / A 1014, 165679 (2021). doi:10.1016/j.nima.2021.165679

Nuclear and High Energy PhysicsParticle physicsPhysics - Instrumentation and DetectorsPhysics::Instrumentation and Detectorsflavor: violation [lepton]FOS: Physical sciencesElectron7. Clean energy01 natural sciences530muon: decayTechnical designMuon decaysHigh Energy Physics - Experimentdesign [detector]High Energy Physics - Experiment (hep-ex)decay [muon]Scintillating tilesPositronsemiconductor detector: pixelScintillating fibres0103 physical sciencesscintillation counter: fibreddc:530tracking detector010306 general physicsInstrumentationEngineering & allied operationsactivity reportdetector: designPhysicspixel [semiconductor detector]MuonPixel010308 nuclear & particles physicsDetectorMonolithic pixel detectorlepton: flavor: violationInstrumentation and Detectors (physics.ins-det)fibre [scintillation counter]sensitivityLepton flavour violationBeamlineHigh Energy Physics::Experimentddc:620performanceLepton
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Radiation hard monolithic CMOS sensors with small electrodes for High Luminosity LHC

2019

Abstract The upgrade of the tracking detectors for the High Luminosity-LHC (HL-LHC) requires the development of novel radiation hard silicon sensors. The development of Depleted Monolithic Active Pixel Sensors targets the replacement of hybrid pixel detectors with radiation hard monolithic CMOS sensors. We designed, manufactured and tested radiation hard monolithic CMOS sensors in the TowerJazz 180 nm CMOS imaging technology with small electrodes pixel designs. These designs can achieve pixel pitches well below current hybrid pixel sensors (typically 50 ×  50 μ m ) for improved spatial resolution. Monolithic sensors in our design allow to reduce multiple scattering by thinning to a total si…

Nuclear and High Energy PhysicsParticle tracking detectors ; Radiation-hard detectors ; Electronic detector readout concepts ; CMOS sensors ; Monolithic active pixel sensorsPhysics::Instrumentation and DetectorscostsRadiationElectronic detector readout concepts01 natural sciences7. Clean energy030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicinesemiconductor detector: pixelElectronic detector readout conceptCMOS sensorselectrode: designParticle tracking detectors0103 physical sciences[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]InstrumentationImage resolutionRadiation hardeningspatial resolutionradiation: damagePhysicsCMOS sensorsemiconductor detector: technologyMonolithic active pixel sensorPixelirradiation010308 nuclear & particles physicsbusiness.industrytracking detector: upgradeDetectorCMOS sensorParticle tracking detectorMonolithic active pixel sensorsUpgradeCERN LHC CollCMOSefficiencyOptoelectronicsbusinessperformanceRadiation-hard detectors
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A New Three-Dimensional Track Fit with Multiple Scattering

2017

Modern semiconductor detectors allow for charged particle tracking with ever increasing position resolution. Due to the reduction of the spatial hit uncertainties, multiple Coulomb scattering in the detector layers becomes the dominant source for tracking uncertainties. In this case long distance effects can be ignored for the momentum measurement, and the track fit can consequently be formulated as a sum of independent fits to hit triplets. In this paper we present an analytical solution for a three-dimensional triplet(s) fit in a homogeneous magnetic field based on a multiple scattering model. Track fitting of hit triplets is performed using a linearization ansatz. The momentum resolution…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsFOS: Physical sciencesTracking (particle physics)01 natural sciencesHigh Energy Physics - Experimentlaw.inventionMomentumHigh Energy Physics - Experiment (hep-ex)OpticsLinearizationlaw0103 physical sciences010306 general physicsColliderInstrumentationAnsatzPhysicsSpectrometer010308 nuclear & particles physicsScatteringbusiness.industryDetectorInstrumentation and Detectors (physics.ins-det)Computational Physics (physics.comp-ph)Computational physicsPhysics - Data Analysis Statistics and ProbabilitybusinessPhysics - Computational PhysicsData Analysis Statistics and Probability (physics.data-an)
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