Search results for "Pixel"

showing 10 items of 421 documents

Digital performance improvements of a CdTe pixel detector for high flux energy-resolved X-ray imaging

2015

Abstract Photon counting detectors with energy resolving capabilities are desired for high flux X-ray imaging. In this work, we present the performance of a pixelated Schottky Al/p-CdTe/Pt detector (4×4) coupled to a custom-designed digital readout electronics for high flux measurements. The detector (4×4×2 mm 3 ) has an anode layout based on an array of 16 pixels with a geometric pitch of 1 mm (pixel size of 0.6 mm). The 4-channel readout electronics is able to continuously digitize and process the signals from each pixel, performing multi-parameter analysis (event arrival time, pulse shape, pulse height, pulse time width, etc.) even at high fluxes and at different throughput and energy re…

PhysicsNuclear and High Energy PhysicsPixelPhysics::Instrumentation and Detectorsbusiness.industryEnergy-resolved photon counting detectorSettore FIS/01 - Fisica SperimentaleDetectorSchottky diodePixel detectorSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Photon countingCharge sharingCdTe detectorHigh photon counting rateFull width at half maximumOpticsDigital pulse processingMonochromatic colorbusinessInstrumentationPulse shape analysiEnergy (signal processing)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Design criteria for multi-layered scintillating fibre arrays with inclined columns

2008

Multi-layered scintillating fibre arrays read-out are commonly used as high resolution charged particle hodoscopes. Fibres of a column along the geometrical trajectory of incident particles are typically grouped to one pixel of a multi-channel read-out device. In some applications the incident particles will cross the detection plane with large angles w.r.t. the normal to the layers. Then, the packing of the fibres needs to be adapted to the incident particles and the columns need to be inclined. In this paper possible fibre array geometries are shown, relevant design criteria for detectors are discussed, and the effect of diverging particles incident on fibre arrays was studied using a Mon…

PhysicsNuclear and High Energy PhysicsPixelPlane (geometry)business.industryMonte Carlo methodDetectorHigh resolutionFOS: Physical sciencesCharged particleOpticsColumn (typography)Scintillating fibreNuclear Experiment (nucl-ex)businessInstrumentationNuclear Experiment
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Laser tests of silicon detectors

2007

This paper collects experiences from the development of a silicon sensor laser testing setup and from tests of silicon strip modules (ATLAS End-cap SCT), pixel modules (DEPFET) and large-area diodes using semiconductor lasers. Lasers of 1060 and 680 nm wavelengths were used. A sophisticated method of focusing the laser was developed. Timing and interstrip properties of modules were measured. Analysis of optical effects involved and detailed discussion about the usability of laser testing for particle detectors are presented.

PhysicsNuclear and High Energy PhysicsPixelSiliconPhysics::Instrumentation and Detectorsbusiness.industryDetectorPhysics::Opticschemistry.chemical_elementLaserlaw.inventionSemiconductor laser theorySemiconductor detectorchemistrylawOptoelectronicsPhysics::Atomic PhysicsbusinessInstrumentationDiodeNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Timing results using an FPGA-based TDC with large arrays of 144 SiPMs

2015

Silicon photomultipliers (SiPMs) have become an alternative to traditional tubes due to several features. However, their implementation to form large arrays is still a challenge especially due to their relatively high intrinsic noise, depending on the chosen readout. In this contribution, two modules composed of SiPMs with an area of roughly mm mm are used in coincidence. Coincidence resolving time (CRT) results with a field-programmable gate array, in combination with a time to digital converter, are shown as a function of both the sensor bias voltage and the digitizer threshold. The dependence of the CRT on the sensor matrix temperature, the amount of SiPM active area and the crystal type…

PhysicsNuclear and High Energy PhysicsPixelbusiness.industryDetectorBiasingNoise (electronics)Time-to-digital converterFull width at half maximumSilicon radiation detectorsSilicon photomultiplierOpticsNuclear Energy and EngineeringGate arrayPositron emission tomography (PET)Nuclear medicineTEORIA DE LA SEÑAL Y COMUNICACIONESElectronic engineeringTrigger circuitsElectrical and Electronic Engineeringbusiness
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Spectroscopic response of a CdZnTe multiple electrode detector

2007

Abstract The spectroscopic performances of a CdZnTe detector (crystal size: 5×5×0.9 mm 3 ) with five electrodes (cathode, anode and three steering electrodes) were studied. The anode layout, which consists of a circular electrode ( φ =80 μm) surrounded by two ring electrodes (gap=100 μm; radial width Δ r =100 μm) and by one electrode that extends to the edge of the crystal, is mostly sensitive to the electron carriers, overcoming the well known effect of the hole trapping in the measured spectra. We report on the spectroscopic response of the detector at different bias voltages of the electrodes and at various photon energies ( 109 Cd, 241 Am and 57 Co sources). The CdZnTe detector exhibits…

PhysicsNuclear and High Energy PhysicsSpectrometerbusiness.industryCdZnTe detectorSteering electrodeDetectorMultiple electrode detectorElectronSmall pixel effectCathodeAnodelaw.inventionCrystalFull width at half maximumX-ray and gamma ray spectroscopylawElectrodeOptoelectronicsbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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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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The track finding algorithm of the Belle II vertex detectors

2017

The Belle II experiment is a high energy multi purpose particle detector operated at the asymmetric e + e − - collider SuperKEKB in Tsukuba (Japan). In this work we describe the algorithm performing the pattern recognition for inner tracking detector which consists of two layers of pixel detectors and four layers of double sided silicon strip detectors arranged around the interaction region. The track finding algorithm will be used both during the High Level Trigger on-line track reconstruction and during the off-line full reconstruction. It must provide good efficiency down to momenta as low as 50 MeV/c where material effects are sizeable even in an extremely thin detector as the VXD. In a…

PhysicsParticle physicsPixel010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsTrack (disk drive)PhysicsQC1-999DetectorCharged particle track finding(all)Tracking (particle physics)01 natural sciencesParticle detectorlaw.inventionMomentumlaw0103 physical sciencesddc:530High Energy Physics::Experiment010306 general physicsColliderAlgorithmEnergy (signal processing)EPJ Web of Conferences
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The Sun as an X‐Ray Star. I. Deriving the Emission Measure Distribution versus Temperature of the Whole Solar Corona from theYohkoh/Soft X‐Ray Telesc…

2000

The scope of this work is to obtain the emission measure distributions versus temperature, EM(T ), of the whole solar corona from Yohkoh Soft X-ray Telescope images. As discussed in Paper II, the EM(T ) is our starting point for studying the Sun as an X-ray star. To this purpose, we need to extract as much information as possible from the Yohkoh/SXT data covering the whole range of the Yohkoh/SXT tem- perature sensitivity, i.e., 5.5 \ log T (K) \ 8. In particular at low photon counts and temperatures below 106 K, errors on the temperature and emission measure determination are expected to be large. To this end, we have made an extensive set of simulations to explore the nominal performance …

PhysicsPhotonPixelGamma rayAstronomy and AstrophysicsAstrophysicsPlasmaMeasure (mathematics)law.inventionTelescopeSpace and Planetary SciencelawRange (statistics)Sensitivity (control systems)The Astrophysical Journal
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Ultra-low material pixel layers for the Mu3e experiment

2016

The upcoming Mu3e experiment will search for the charged lepton flavour violating decay of a muon at rest into three electrons. The maximal energy of the electrons is 53 MeV, hence a low material budget is a key performance requirement for the tracking detector. In this paper we summarize our approach to meet the requirement of about 0.1 % of a radiation length per pixel detector layer. This includes the choice of thinned active monolithic pixel sensors in HV-CMOS technology, ultra-thin flexible printed circuits, and helium gas cooling.

PhysicsPhysics - Instrumentation and DetectorsMuonPixel010308 nuclear & particles physicsbusiness.industryPhysics::Instrumentation and DetectorsDetectorComputingMethodologies_IMAGEPROCESSINGANDCOMPUTERVISIONFOS: Physical sciencesElectronInstrumentation and Detectors (physics.ins-det)Tracking (particle physics)01 natural sciencesRadiation lengthPrinted circuit boardOptics0103 physical sciencesHigh Energy Physics::Experiment010306 general physicsbusinessInstrumentationMathematical PhysicsLepton
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MuPix7 - A fast monolithic HV-CMOS pixel chip for Mu3e

2016

The MuPix7 chip is a monolithic HV-CMOS pixel chip, thinned down to 50 \mu m. It provides continuous self-triggered, non-shuttered readout at rates up to 30 Mhits/chip of 3x3 mm^2 active area and a pixel size of 103x80 \mu m^2. The hit efficiency depends on the chosen working point. Settings with a power consumption of 300 mW/cm^2 allow for a hit efficiency >99.5%. A time resolution of 14.2 ns (Gaussian sigma) is achieved. Latest results from 2016 test beam campaigns are shown.

PhysicsPhysics - Instrumentation and DetectorsPixel010308 nuclear & particles physicsbusiness.industryGaussianFOS: Physical sciencesTime resolutionInstrumentation and Detectors (physics.ins-det)Semiconductor deviceChip01 natural sciencessymbols.namesakeCMOSTest beam0103 physical sciencessymbolsOptoelectronicsddc:610010306 general physicsbusinessInstrumentationGaussian processMathematical Physics
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