Search results for "pixel [semiconductor detector]"

showing 10 items of 79 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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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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Technical design report for the upgrade of the ALICE inner tracking system

2014

ALICE (A Large Ion Collider Experiment) is studying the physics of strongly interacting matter, and in particular the properties of the Quark–Gluon Plasma (QGP), using proton–proton, proton–nucleus and nucleus–nucleus collisions at the CERN LHC (Large Hadron Collider). The ALICE Collaboration is preparing a major upgrade of the experimental apparatus, planned for installation in the second long LHC shutdown in the years 2018–2019. A key element of the ALICE upgrade is the construction of a new, ultra-light, high- resolution Inner Tracking System (ITS) based on monolithic CMOS pixel detectors. The primary focus of the ITS upgrade is on improving the performance for detection of heavy-flavour…

ROOT-S=2.76 TEV; PP COLLISIONS; DETECTORS; RECONSTRUCTION; ELECTRONICS; SILICON; PHYSICS; MODELPhysics::Instrumentation and DetectorsNuclear TheoryNuclear and High Energy Physics;Tracking (particle physics)01 natural sciences7. Clean energydecaylaw.inventionUpgradeALICElawLHC; ALICE; Inner Tracking SystemNuclear ExperimentGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)ComputingMilieux_MISCELLANEOUSPhysicsLarge Hadron ColliderDetectorSettore FIS/01 - Fisica SperimentaleTracking systemPRIRODNE ZNANOSTI. Fizika.UpgradeLHCParticle physicsNuclear and High Energy PhysicsALICE Inner Tracking SystemROOT-S=2.76 TEV; pp collisions; DETECTORS; RECONSTRUCTION; ELECTRONICS; SILICON; PHYSICS; MODEL; decay[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Dot pitchPHYSICSELECTRONICS0103 physical sciencesDETECTORSRECONSTRUCTIONCMOS pixel sensors010306 general physicsColliderROOT-S=2.76 TEVSILICONPP COLLISIONSPixel010308 nuclear & particles physicsbusiness.industryALICE experimentInner Tracking SystemTechnical Design ReportNATURAL SCIENCES. Physics.MODELDetector upgradeTechnical Design Report; Upgrade; ALICE Inner Tracking SystemHigh Energy Physics::Experimentbusiness
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Efficient smart-camera accelerator: A configurable motion estimator dedicated to video codec

2013

Smart cameras are used in a large range of applications. Usually the smart cameras transmit the video or/and extracted information from the video scene, frequently on compressed format to fit with the application requirements. An efficient hardware accelerator that can be adapted and provide the required coding performances according to the events detected in the video, the available network bandwidth or user requirements, is therefore a key element for smart camera solutions. We propose in this paper to focus on a key part of the compression system: motion estimation. We have developed a flexible hardware implementation of the motion estimator based on FPGA component, fully compatible with…

Motion compensationHardware and ArchitectureComputer scienceMotion estimationReal-time computingHardware accelerationCodecSmart cameraField-programmable gate arraySoftwareQuarter-pixel motionBlock-matching algorithmJournal of Systems Architecture
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Formation of real, orthoscopic integral images by smart pixel mapping.

2005

Integral imaging systems are imaging devices that provide 3D images of 3D objects. When integral imaging systems work in their standard configuration the provided reconstructed images are pseudoscopic; that is, are reversed in depth. In this paper we present, for the first time we believe, a technique for formation of real, undistorted, orthoscopic integral images by direct pickup. The technique is based on a smart mapping of pixels of an elemental-images set. Simulated imaging experiments are presented to support our proposal.

Set (abstract data type)Integral imagingOpticsPixelbusiness.industryComputer sciencePixel mappingComputingMethodologies_IMAGEPROCESSINGANDCOMPUTERVISIONImaging sciencebusinessImage resolutionAtomic and Molecular Physics and OpticsOptics express
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Electrical Characterization of CdTe pixel detectors with Al Schottky anode

2014

Abstract Pixelated Schottky Al/p-CdTe/Pt detectors are very attractive devices for high-resolution X-ray spectroscopic imaging, even though they suffer from bias-induced time instability (polarization). In this work, we present the results of the electrical characterization of a (4×4) pixelated Schottky Al/p-CdTe/Pt detector. Current–voltage ( I–V ) characteristics and current transients were investigated at different temperatures. The results show deep levels that play a dominant role in the charge transport mechanism. The conduction mechanism is dominated by the space charge limited current (SCLC) both under forward bias and at high reverse bias. Schottky barrier height of the Al/CdTe con…

PhysicspolarizationNuclear and High Energy PhysicsSchottky contactbusiness.industrySchottky barrierSettore FIS/01 - Fisica SperimentaleSchottky diodeCdTeThermal conductionSpace chargeCadmium telluride photovoltaicsSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Settore FIS/03 - Fisica Della MateriaAnodeX-ray and gamma ray spectroscopypixel detectorOptoelectronicsPolarization (electrochemistry)businessCdTe; Schottky contacts; polarization; pixel detectors; X-ray and gamma ray spectroscopyInstrumentationVoltage
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Technical design of the phase I Mu3e experiment

2021

Nuclear instruments & 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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The Wide Field Imager instrument for Athena

2017

ESA's next large X-ray mission ATHENA is designed to address the Cosmic Vision science theme 'The Hot and Energetic Universe'. It will provide answers to the two key astrophysical questions how does ordinary matter assemble into the large-scale structures we see today and how do black holes grow and shape the Universe. The ATHENA spacecraft will be equipped with two focal plane cameras, a Wide Field Imager (WFI) and an X-ray Integral Field Unit (X-IFU). The WFI instrument is optimized for state-of-The-Art resolution spectroscopy over a large field of view of 40 amin x 40 amin and high count rates up to and beyond 1 Crab source intensity. The cryogenic X-IFU camera is designed for high-spect…

Hot and Energetic UniverseX-ray detector.Electronic Optical and Magnetic MaterialFocal plane cameraComputer Science Applications1707 Computer Vision and Pattern RecognitionCondensed Matter Physic02 engineering and technology021001 nanoscience & nanotechnology01 natural sciencesX-ray astronomyApplied Mathematic010309 opticsActive pixel sensorSettore FIS/05 - Astronomia E AstrofisicaWFI0103 physical sciencesAthenaElectrical and Electronic Engineering0210 nano-technologyDEPFETUV, X-Ray, and Gamma-Ray Space Instrumentation for Astronomy XX
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High-resolution far-field integral-imaging camera by double snapshot

2012

In multi-view three-dimensional imaging, to capture the elemental images of distant objects, the use of a field-like lens that projects the reference plane onto the microlens array is necessary. In this case, the spatial resolution of reconstructed images is equal to the spatial density of microlenses in the array. In this paper we report a simple method, based on the realization of double snapshots, to double the 2D pixel density of reconstructed scenes. Experiments are reported to support the proposed approach.

Computer scienceMotion PicturesComputingMethodologies_IMAGEPROCESSINGANDCOMPUTERVISIONNear and far fieldlaw.inventionImaging Three-DimensionalOpticslawPhotographyHumansImage resolutionFatigueLensesMicrolensDepth PerceptionIntegral imagingbusiness.industryPhotographyAccommodation OcularEquipment DesignConvergence OcularAtomic and Molecular Physics and OpticsLens (optics)Computer Science::Computer Vision and Pattern RecognitionDepth perceptionbusinessAlgorithmsPixel densityOptics Express
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Charge loss correction in CZT pixel detectors at low and high fluxes: analysis of positive and negative pulses

2018

Charge losses are typical drawbacks in cadmium–zinc–telluride (CZT) pixel detectors. The effects of these phenomena are strongly related to the interaction point of the photons and are more severe for photon interactions at the inter-pixel gap and near the pixelated anode. In this work, we present some original techniques able to correct charge losses in pixelated CZT detectors at both low and high fluxes. The height, the shape and the arrival time of collected- and induced-charge pulses with both positive and negative polarities are analysed to recover charge losses after the application of charge sharing addition (CSA). Sub-millimetre CZT pixel detectors, fabricated by different manufactu…

Settore FIS/01 - Fisica SperimentaleCZT pixel detectors Charge sharing Charge losses Charge loss correction negative induced-charge pulsesSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)
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