Search results for "Image resolution"

showing 10 items of 377 documents

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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Detector blockbased on arrays of 144 SiPMs and monolithic scintillators: A performane study

2015

[EN] We have developed a detector block composed by a monolithic LYSO scintillator coupled to a custom made 12 12 SiPMs array. The design is mainly focused to applications such as Positron Emission Tomography. The readout electronics is based on 3 identical and scalable Application Specific Integrated Circuits (ASIC). We have determined the main performance of the detector block namely spatial, energy, and time resolution but also the system capability to determine the photon depth of interaction, for different crystal surface treatments. Intrinsic detector spatial resolution values as good as 1.7 mm FWHM and energies of 15% for black painted crystals were measured. & 2014 Elsevier B.V. All…

PhysicsNuclear and High Energy Physicsmedicine.medical_specialtyPhotonPhysics::Instrumentation and Detectorsbusiness.industryASICDetectorSilicon photomultipliersScintillatorScintillator crystalFull width at half maximumSilicon photomultiplierApplication-specific integrated circuitmedicineOptoelectronicsMedical physicsbusinessMATEMATICA APLICADAInstrumentationImage resolutionPositron Emission TomographyBlock (data storage)
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Development of silicon pad detectors and readout electronics for a Compton camera

2003

Abstract Applications in nuclear medicine and bio-medical engineering may profit using a Compton camera for imaging distributions of radio-isotope labelled tracers in organs and tissues. These applications require detection of photons using thick position-sensitive silicon sensors with the highest possible energy and good spatial resolution. In this paper, research and development on silicon pad sensors and associated readout electronics for a Compton camera are presented. First results with low-noise, self-triggering VATAGP ASIC's are reported. The measured energy resolution was 1.1 keV FWHM at room temperature for the 241 Am photo-peak at 59.5 keV .

PhysicsNuclear and High Energy Physicsmedicine.medical_specialtyPhotonSiliconPhysics::Instrumentation and Detectorsbusiness.industryAstrophysics::High Energy Astrophysical PhenomenaDetectorCompton scatteringchemistry.chemical_elementParticle detectorSemiconductor detectorOpticschemistryMeasuring instrumentmedicineMedical physicsbusinessInstrumentationImage resolutionNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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A prototype of very high resolution small animal PET scanner using silicon pad detectors

2007

Abstract A very high-resolution small animal positron emission tomograph (PET), which can achieve sub-millimeter spatial resolution, is being developed using silicon pad detectors. The prototype PET for a single slice instrument consists of two 1 mm thick silicon pad detectors, each containing a 32×16 array of 1.4×1.4 mm pads readout with four VATAGP3 chips which have 128 channels low-noise self-triggering ASIC in each chip, coincidence units, a source turntable and tungsten slice collimator. The silicon detectors were located edgewise on opposite sides of a 4 cm field-of-view to maximize efficiency. Energy resolution is dominated by electronic noise, which is 0.98% (1.38 keV) FWHM at 140.5…

PhysicsNuclear and High Energy Physicsmedicine.medical_specialtySiliconbusiness.industryDetectorResolution (electron density)chemistry.chemical_elementCollimatorChipLine sourceArticlelaw.inventionOpticschemistrylawmedicineWaferMedical physicsbusinessInstrumentationImage resolution
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Continuously Variable Periodic Test Target

1987

CONTINUOUSLY VARIABLE PERIODIC TEST TARGETP. ANDRES*, J. OJEDA- CASTANEDAt, and J.C. BARREIRO*tINAOE, Apartado Postal 216, 72000 Puebla, Pue., Mexico*Departamento de Optica, Universidad de Valencia, 46100 Burjasot, Spain1. INTRODUCTIONThe modulus of the optical transfer function (MTF) of the eye or any other optical system is usuallyevaluated by imaging either several gratings each with different spatial frequency, or a single test tar-get having patterns with different frequencies (USAF resolution chart). In any of these two usual proce-dures, the measurement of the MTF is made at discrete values of the spatial frequency.Here we describe a method based on the self -imaging phenomenon for p…

PhysicsOptical axisOpticsbusiness.industryOptical transfer functionTalbot effectImage processingSpatial frequencyMonochromatic colorGratingbusinessImage resolutionSPIE Proceedings
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Diffractive optics for high-resolution low-coherence digital holography

2010

We study the properties of the recording of off-axis holograms when a 10 fs pulsed laser is used as illumination source. A proper optical design involving one diffractive lens outside a Michelson interferometer enables the recording of full-field off-axis holograms with high resolution and optical sectioning. We demonstrate our approach with some experimental results that show optical sectioning with a maximum resolution of 3.5 µm. We note that the axial resolution of the technique is reduced up to 9 µm when the object beam travels through a few millimeters of glass due to the pulse broadening along dispersive media.

PhysicsOptical sectioningbusiness.industryHolographyPhysics::OpticsMichelson interferometerHolographic interferometrylaw.inventionInterferometryOpticslawOptoelectronicsbusinessImage resolutionDigital holographyCoherence (physics)2010 9th Euro-American Workshop on Information Optics
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Resistive Micromegas for the Muon Spectrometer Upgrade of the ATLAS Experiment

2017

It is reported on the construction and test of large scale resistive Micromegas detectors for the ATLAS New Small Wheel upgrade. The production procedure of the 2 to 3 m2 active area is described. The validation of the construction procedure is proven with results obtained with prototype detectors showing 100 µm spatial resolution in the precision coordinate and above 98% efficiency In the context of the upgrade project of the ATLAS Muon system, we report on the construction of Micromegas detectors with an active area of 2 to 3 m$^2$ . The validation of the construction procedure is proven with results obtained with prototype detectors showing 100 $\mu $m spatial resolution in the precision…

PhysicsParticle physicsMuonPhysics::Instrumentation and DetectorsATLAS experimentDetectorContext (language use)MicroMegas detectorNuclear physicsmedicine.anatomical_structureUpgradeAtlas (anatomy)medicineHigh Energy Physics::ExperimentImage resolutionParticle Physics - Experiment
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DOI measurement with monolithic scintillation crystals: A primary performance evaluation

2007

We report a first assessment of image quality enhancement achieved by the implementation of depth of interaction detection with monolithic crystals. The method of interaction depth measurement is based on analogue computation of the standard deviation with an enhanced charge divider readout. This technique of depth of interaction detection was developed in order to provide fast and determination of this parameter at a reasonable increase of detector cost. The detector consists of an large-sized monolithic scintillator coupled to a position sensitive photomultiplier tube. A special design feature is the flat-topped pyramidal shape of the crystal. This reduces image compression near the edges…

PhysicsPhotomultiplierOpticsPhysics::Instrumentation and DetectorsImage qualityPoint sourcebusiness.industryMeasured depthDetectorScintillatorbusinessImage resolutionImaging phantom2007 IEEE Nuclear Science Symposium Conference Record
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Monte Carlo and experimental derivation of TG43 dosimetric parameters for CSM-type Cs-137 sources

2004

In this study, complete dosimetric datasets for the CSM2 and CSM3 Cs-137 sources were obtained using the Monte Carlo GEANT4 code. The application of this calculation method was experimentally validated with thermoluminescent dosimetry (TLD). Functions and parameters following the TG43 formalism are presented: the dose rate constant, the radial dose functional, and the anisotropy function. In addition, to aid the quality control process on treatment planning systems, a two-dimensional (2D) rectangular dose rate table (the traditional along-away table), coherent with the TG43 dose calculation formalism, is given. The data given in this study complement existing information for both sources on…

PhysicsPhotonmedia_common.quotation_subjectPhysics::Medical PhysicsMonte Carlo methodGeneral MedicineAsymmetryThermoluminescent DosimetryDosimetryStatistical physicsThermoluminescent dosimeterAnisotropyImage resolutionmedia_commonMedical Physics
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