Search results for "techniques"

showing 10 items of 4426 documents

Silicon detector for a Compton camera in nuclear medical imaging

2002

Electronically collimated gamma ca\-me\-ras based on Com\-pton scattering in silicon pad sensors may improve imaging in nuclear medicine and bio-medical research. The work described here concentrates on the silicon pad detector developed for a prototype Compton camera. The silicon pad sensors are read out using low noise VLSI CMOS chips and novel fast triggering chips. Depending on the application a light weight and dense packaging of sensors and its readout electronics on a hybrid is required. We describe the silicon pad sensor and their readout with the newly designed hybrid. %The silicon detector of a Compton camera %may contain up to $10^5$~analogue channels requiring %a fast and low co…

PhysicsNuclear and High Energy PhysicsSiliconbusiness.industryPhysics::Instrumentation and DetectorsAstrophysics::High Energy Astrophysical PhenomenaDetectorCompton scatteringchemistry.chemical_elementChipCollimated lightData acquisitionNuclear Energy and EngineeringCMOSchemistryElectronic engineeringOptoelectronicsElectrical and Electronic EngineeringImage sensorDetectors and Experimental Techniquesbusiness
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Triple GEM tracking detectors for COMPASS

2002

The small area tracker of COMPASS, a high-luminosity fixed target experiment at CERN's SPS, includes a set of 20 large-size ($31\times 31\,\cm^2$) Gas Electron Multiplier (GEM) detectors. Based on gas amplification in three cascaded GEM foils, these devices permit to obtain high gain and good spatial resolution even at very high particle fluxes. A two-coordinate projective readout yields, for each track, highly correlated signal amplitudes on both projections, allowing to resolve multiple hits in high occupancy regions close to the central deactivated area of $5\,\cm$ diameter. At the same time the material exposed to the beam is minimized. Splitting the amplification in three cascaded stag…

PhysicsNuclear and High Energy PhysicsSpectrometerPhysics::Instrumentation and Detectorsbusiness.industryDetectorTracking (particle physics)Nuclear physicsOpticsNuclear Energy and EngineeringCompassNuclear electronicsGas electron multiplierDetectors and Experimental TechniquesElectrical and Electronic EngineeringbusinessImage resolutionBeam (structure)IEEE Transactions on Nuclear Science
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Performance of long modules of silicon microstrip detectors

1998

This note describes the performance of modules assembled with up to twelve silicon microstrip detectors. These modules were built for the instrumented Silicon Target (STAR) that has been installed in the NOMAD spectrometer. Laboratory and test beam results are compared with model predictions. For a module of nine detectors, test beam results indicate a signal--to--noise ratio of 19, a hit finding efficiency of 99.8\% and a spatial resolution of 6.0 $\mu$m. Laboratory measurements indicate that modules of twelve detectors exhibit a signal--to--noise ratio of the order of 16.

PhysicsNuclear and High Energy PhysicsSpectrometerSiliconbusiness.industryPhysics::Instrumentation and DetectorsDetectorchemistry.chemical_elementFísicaParticle detectorSemiconductor detectorNuclear physicssilicon microstrip detectors; neutrino oscillationsSignal-to-noise ratioOpticschemistryMeasuring instrumentHigh Energy Physics::ExperimentDetectors and Experimental TechniquesbusinessInstrumentationImage resolution
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PERFORMANCE OF THE ALEPH TIME PROJECTION CHAMBER

1991

The performance of the ALEPH Time Projection Chamber (TPC) has been studied using data taken during the LEP running periods in 1989 and 1990. After correction of residual distortions and optimisation of coordinate reconstruction algorithms, single coordinate resolutions of 173-mu-m in the azimuthal and 740-mu-m in the longitudinal direction are achieved. This results in a momentum resolution for the TPC of DELTA-p/p2 = 1.2 x 10(-3) (GeV/c)-1. In combination with the ALEPH Inner Tracking Chamber (ITC), a total momentum resolution of DELTA-p/p2 = 0.8 x 10(-3) (GeV/c)-1 is obtained. With respect to particle identification, the detector achieves a resolution of 4.4% for the measurement of the i…

PhysicsNuclear and High Energy PhysicsTime projection chamberPhysics::Instrumentation and DetectorsTracking (particle physics)Particle identificationParticle detectorMomentumNuclear physicsAzimuthPair productionHigh Energy Physics::ExperimentDetectors and Experimental TechniquesInstrumentationImage resolution
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Electron-pion discrimination with a scintillating fiber calorimeter

1990

Abstract We report on an experimental study of a variety of techniques for discriminating between (isolated) electrons and pions in a lead and scintillating fiber calorimeter without longitudinal segmentation. Using information from the lateral shower development, from a pre-shower detector, from the time structure of the signals, or from a combination of these we measure pion rejection factors of up to several thousand while maintaining electron efficiencies of 95% or higher.

PhysicsNuclear and High Energy Physicsintegumentary systemCalorimeter (particle physics)BackscatterScintillating fiberPhysics::Instrumentation and Detectorsbusiness.industryDetectorElectronNuclear physicsOpticsPionHigh Energy Physics::ExperimentTime structureDetectors and Experimental Techniquesbusinesshuman activitiesInstrumentation
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A decade of SN 1993J : discovery of radio wavelength effects in the expansion rate

2009

We studied the growth of the shell-like radio structure of supernova SN 1993J in M 81 from September 1993 to October 2003 with very-long-baseline interferometry (VLBI) observations at the wavelengths of 3.6, 6, and 18 cm. We developed a method to accurately determine the outer radius (R) of any circularly symmetric compact radio structure such as SN 1993J. The source structure of SN 1993J remains circularly symmetric (with deviations from circularity under 2%) over almost 4000 days. We characterize the decelerated expansion of SN 1993J until approximately day 1500 after explosion with an expansion parameter m = 0.845 ± 0.005 (R ∝ tm). However, from that day onwards the expansion differs whe…

PhysicsOpacitygeneral [Supernovae]Astronomy and AstrophysicsRadiusAstrophysics:ASTRONOMÍA Y ASTROFÍSICA::Cosmología y cosmogonia::Galaxias [UNESCO]clusters : individual : M 81 [Galaxies]Magnetic fieldInterpretation (model theory)SupernovaWavelengthGalaxies : clusters : individual : M 81; Radio continuum : stars; Supernovae : general; Supernovae : individual : SN 1993J; Techniques : interferometricSpace and Planetary ScienceVery-long-baseline interferometryinterferometric [Techniques]stars [Radio continuum]UNESCO::ASTRONOMÍA Y ASTROFÍSICA::Cosmología y cosmogonia::Estrellasindividual : SN 1993J [Supernovae]EjectaUNESCO::ASTRONOMÍA Y ASTROFÍSICA::Cosmología y cosmogonia::Galaxias:ASTRONOMÍA Y ASTROFÍSICA::Cosmología y cosmogonia::Estrellas [UNESCO]
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The MuPix high voltage monolithic active pixel sensor for the Mu3e experiment

2015

Mu3e is a novel experiment searching for charged lepton flavor violation in the rare decay μ → eee. In order to reduce background by up to 16 orders of magnitude, decay vertex position, decay time and particle momenta have to be measured precisely. A pixel tracker based on 50 μm thin high voltage monolithic active pixel sensors (HV-MAPS) in a magnetic field will deliver precise vertex and momentum information. Test beam results like an excellent efficiency of >99.5% and a time resolution of better than 16.6 ns obtained with the MuPix HV-MAPS chip developed for the Mu3e pixel tracker are presented.

PhysicsParticle physicsCMOS sensorElectronic detector readout concepts (solid-state)PixelPhysics::Instrumentation and Detectorsbusiness.industryHigh voltageChipElectronic detector readout concepts (solid-state); Particle tracking detectors (solidstate detectors)Magnetic fieldVertex (geometry)OpticsHigh Energy Physics::Experimentddc:610Electric potentialDetectors and Experimental TechniquesParticle tracking detectors (solidstate detectors)ddc:620businessInstrumentationParticle Physics - ExperimentMathematical PhysicsEngineering & allied operationsLepton
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Topological and Central Trigger Processor for 2014 LHC luminosities

2012

The ATLAS experiment is located at the European Center for Nuclear Research (CERN) in Switzerland. It is designed to observe phenomena that involve highly massive particles produced in the collisions at the Large Hadron Collider (LHC): the world’s largest and highest-energy particle accelerator. Event triggering and Data Acquisition is one of the extraordinary challenges faced by the detectors at the high luminosity LHC collider. During 2011, the LHC reached instantaneous luminosities of 4 10^33 cm−1 s−1 and produced events with up to 24 interactions per colliding proton bunch. This places stringent operational and physical requirements on the ATLAS Trigger in order to reduce the 40MHz coll…

PhysicsParticle physicsLarge Hadron ColliderLuminosity (scattering theory)Physics::Instrumentation and DetectorsATLAS experimentParticle acceleratorlaw.inventionNuclear physicsUpgradelawNuclear electronicsPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentDetectors and Experimental TechniquesNuclear ExperimentColliderEvent (particle physics)
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MoEDAL: Seeking magnetic monopoles and more at the LHC

2015

The MoEDAL experiment (Monopole and Exotics Detector at the LHC) is designed to directly search for magnetic monopoles and other highly ionising stable or metastable particles arising in various theoretical scenarios beyond the Standard Model. Its physics goals --largely complementary to the multi-purpose LHC detectors ATLAS and CMS-- are accomplished by the deployment of plastic nuclear track detectors combined with trapping volumes for capturing charged highly ionising particles and TimePix pixel devices for monitoring. This paper focuses on the status of the detectors and the prospects for LHC Run II.

PhysicsParticle physicsLarge Hadron ColliderPhysics - Instrumentation and DetectorsPhysics::Instrumentation and DetectorsPhysics beyond the Standard ModelDetectorMagnetic monopoleFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)High Energy Physics - ExperimentHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenologymedicine.anatomical_structureMoEDAL experimentHigh Energy Physics - Phenomenology (hep-ph)Nuclear trackAtlas (anatomy)medicineDetectors and Experimental Techniques
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Upgrade of the ATLAS Level-1 trigger with an FPGA based Topological Processor

2013

The ATLAS experiment is located at the European Centre for Nuclear Research (CERN) in Switzerland. It is designed to measure decay properties of high energetic particles produced in the protons collisions at the Large Hadron Collider (LHC). The LHC has a proton collision at a frequency of 40 MHz, and thus requires a trigger system to efficiently select events down to a manageable event storage rate of about 400Hz. Event triggering is therefore one of the extraordinary challenges faced by the ATLAS detector. The Level-1 Trigger is the first rate-reducing step in the ATLAS Trigger, with an output rate of 75kHz and decision latency of less than 2.5$\mu$s. It is primarily composed of the Calori…

PhysicsParticle physicsLarge Hadron ColliderPhysics::Instrumentation and DetectorsNuclear TheoryATLAS experimentUpgrademedicine.anatomical_structureAtlas (anatomy)Optical receiversmedicinePhysics::Accelerator PhysicsSignal processing algorithmsHigh Energy Physics::ExperimentDetectors and Experimental TechniquesNuclear ExperimentField-programmable gate array
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