Search results for "SIMULATION"

showing 10 items of 5095 documents

Twofold coordinated Ge defects induced by gamma-ray irradiation in Ge-doped SiO2

2008

We report an experimental study by photoluminescence, optical absorption and Electron Paramagnetic Resonance measurements on the effects of exposure of Ge-doped amorphous SiO2 to gamma ray radiation at room temperature. We have evidenced that irradiation at doses of the order of 1 MGy is able to generate Ge-related defects, recognizable from their optical properties as twofold coordinated Ge centers. Until now, such centers, responsible for photosensitivity of Ge-doped SiO2, have been induced only in synthesis procedures of materials. The found result evidences a role played by gamma radiation in generating photosensitive defects and could furnish a novel basis for photosensitive pattern wr…

PhotoluminescenceMaterials sciencesistemi amorfi difetti di puntoRadiationIonizing radiationlaw.inventionOpticsPhotosensitivitylawFiber Optic TechnologyComputer SimulationIrradiationElectron paramagnetic resonanceGe defectsLightingbusiness.industryGermaniumGamma rayEquipment DesignModels TheoreticalSilicon DioxideAtomic and Molecular Physics and OpticsAmorphous solidEquipment Failure AnalysisGamma Raysgamma-ray irradiationComputer-Aided DesignSiO2business
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Time of flight measurements based on FPGA using a breast dedicated PET

2014

In this work the implementation of a Time-to-Digital Converter (TDC) using a Nutt delay line FPGA-based and applied on a Positron Emission Tomography (PET) device is going to be presented in order to check the system’s suitability for Time of Flight (TOF) measurements. In recent years, FPGAs have shown great advantages for precise time measurements in PET. The architecture employed for these measurements is described in detail. The system developed was tested on a dedicated breast PET prototype, composed of LYSO crystals and Positive Sensitive Photomultipliers (PSPMTs). Two distinct experiments were carried out for this purpose. In the first test, system linearity was evaluated in order to …

PhotomultiplierImage qualityComputer scienceInstrumentation and methods for time-of-flight (TOF) spectroscopyLinearityTrigger detectorsCoincidenceLyso-Time of flightLine (geometry)TEORIA DE LA SEÑAL Y COMUNICACIONESField-programmable gate arrayInstrumentationMathematical PhysicsSimulation
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Comments on 'SPICE Model of Photomultiplier Tube Under Different Bias Conditions'

2021

[EN] The paper ¿SPICE Model of Photomultiplier Tube Under Different Bias Conditions¿ is commented. We revisit the mathematical formulation to compensate for some ambiguities in the original manuscript, and point out some inconsistencies in the results and reproducibility of the simulations, as well as in the optimized parameters originally obtained with the PSPICE simulation engine. All simulations are recalculated with the NGSPICE software using the corrected parameters and compared against the original figures. The reproducibility of our simulations is independently verified with PSPICE, as well as by numerically solving the analytical system of non-linear equations using Newton¿s method …

PhotomultiplierReproducibilityComputer sciencebusiness.industrySpiceModels matemàticsNumerical modelsSoftwareFISICA APLICADAPoint (geometry)Electrical and Electronic EngineeringMATLABbusinessMATEMATICA APLICADAInstrumentationcomputerSimulationcomputer.programming_language
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Sensitivity of alanine dosimeters with gadolinium exposed to 6 MV photons at clinical doses.

2011

In this study we analyzed the ESR signal of alanine dosimeters with gadolinium exposed to 6 MV linear accelerator photons. We observed that the addition of gadolinium brings about an improvement in the sensitivity to photons because of its high atomic number. The experimental data indicated that the addition of gadolinium increases the sensitivity of the alanine to 6 MV photons. This enhancement was better observed at high gadolinium concentrations for which the tissue equivalence is heavily reduced. However, information about the irradiation setup and of the radiation beam features allows one to correct for this difference. Monte Carlo simulations were carried out to obtain information on …

PhotonESR dosimetryGadoliniumMonte Carlo methodAccelerationBiophysicschemistry.chemical_elementGadoliniumLinear particle acceleratorRadiology Nuclear Medicine and imagingIrradiationRadiometryMonte Carlo simulationAlaninePhotonsRadiationDosimeterAlanineChemistryX-RaysRadiochemistryElectron Spin Resonance SpectroscopyDose-Response Relationship RadiationSettore FIS/07 - Fisica Applicata(Beni Culturali Ambientali Biol.e Medicin)Alanine dosimeters gadoliniumLinear ModelsSensitivity (electronics)Monte Carlo MethodRadiation research
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Electronic Excitation Energy Transfer between Two Single Molecules Embedded in a Polymer Host

2007

Unidirectional electronic excitation energy transfer from a photoexcited donor chromophore to a ground state acceptor chromophore - both linked by a rigid bridge - has been investigated by low temperature high-resolution single molecule spectroscopy. Our approach allows for accurately accessing static disorder in the donor and acceptor electronic transitions and to calculate the spectral overlap for each couple. By plotting the experimentally determined transfer rates against the spectral overlap, we can distinguish and quantify Förster- and non-Förster-type contributions to the energy transfer.

PhotonMaterials scienceGeneral Physics and Astronomy02 engineering and technologyImides010402 general chemistry01 natural sciences7. Clean energyCondensed Matter::Materials ScienceFluorescence Resonance Energy TransferPolymethyl MethacrylateMoleculeComputer SimulationPhysics::Chemical Physicschemistry.chemical_classificationPhotonsQuantitative Biology::BiomoleculesPhysics::Biological PhysicsPolymerChromophore021001 nanoscience & nanotechnologyAcceptor0104 chemical sciencesEnergy TransferModels ChemicalchemistryAtomic electron transition[PHYS.PHYS.PHYS-CHEM-PH]Physics [physics]/Physics [physics]/Chemical Physics [physics.chem-ph]Atomic physics0210 nano-technologyGround stateExcitationPhysical Review Letters
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A study of the material in the ATLAS inner detector using secondary hadronic interactions

2011

The ATLAS inner detector is used to reconstruct secondary vertices due to hadronic interactions of primary collision products, so probing the location and amount of material in the inner region of ATLAS. Data collected in 7 TeV pp collisions at the LHC, with a minimum bias trigger, are used for comparisons with simulated events. The reconstructed secondary vertices have spatial resolutions ranging from ~ 200μm to 1 mm. The overall material description in the simulation is validated to within an experimental uncertainty of about 7%. This will lead to a better understanding of the reconstruction of various objects such as tracks, leptons, jets, and missing transverse momentum.

PhotonPhysics::Instrumentation and Detectorsdetector modelling and simulations i (interaction of radiation with matter; interaction; large detector systems for particle and astroparticle physics; of photons with matter; interaction of hadrons with matter; etc); particle tracking detectors (solid-state detectors); si microstrip and pad detectors01 natural sciencesparticle tracking detectors[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]of photons with matter interaction of hadrons with matter etc)InstrumentationGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)Detectors de radiacióMathematical PhysicsPhysicsDetector modelling and simulations I (interaction of radiation with matter interaction of photons with matter interaction of hadrons with matter etc)Large Hadron ColliderSettore FIS/01 - Fisica SperimentaleDetectorVERTEX DETECTORSSi microstrip and pad detectorsTransition radiation detectorinteraction of hadrons with matterExperimental uncertainty analysismedicine.anatomical_structureParticle tracking detectors (Solid-state detectors)Física nuclearParticle Physics - Experimentof photons with matterParticle physicsDetector modelling and simulations I (interaction of radiation with matter interaction of photons with matter interaction of hadrons with matter etc); Particle tracking detectors (Solid-state detectors); Si microstrip and pad detectors; Large detector systems for particle and astroparticle physicsCiências Naturais::Ciências Físicas:Ciências Físicas [Ciências Naturais]Detector modelling and simulations I (interaction of radiation with matter interactionDetector modelling and simulations I (interaction of radiation with matterddc:500.2530Detector Modelling and SimulationsInteraction of photons with matterNuclear physicsAtlas (anatomy)0103 physical sciencesmedicineddc:610010306 general physicsetc)Astroparticle physicsParticle Tracking DetectorsScience & Technology010308 nuclear & particles physicsLarge detector systems for particle and astroparticle physicsLarge Detector Systemsdetector modelling and simulations IFísicaCol·lisions (Física nuclear)Experimental High Energy PhysicsHigh Energy Physics::ExperimentSi Microstrip and Pad DetectorsLepton
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The FiR 1 photon beam model adjustment according to in-air spectrum measurements with the Mg(Ar) ionization chamber.

2014

Abstract The mixed neutron–photon beam of FiR 1 reactor is used for boron–neutron capture therapy (BNCT) in Finland. A beam model has been defined for patient treatment planning and dosimetric calculations. The neutron beam model has been validated with an activation foil measurements. The photon beam model has not been thoroughly validated against measurements, due to the fact that the beam photon dose rate is low, at most only 2% of the total weighted patient dose at FiR 1. However, improvement of the photon dose detection accuracy is worthwhile, since the beam photon dose is of concern in the beam dosimetry. In this study, we have performed ionization chamber measurements with multiple b…

PhotonQuantitative Biology::Tissues and OrgansPhysics::Medical PhysicsMonte Carlo methodAnalytical chemistryBoron Neutron Capture TherapySensitivity and SpecificityOpticsNuclear ReactorsDosimetryPenelopeIonization ChamberDosimetryComputer SimulationPhoton beamRadiometryMonte CarloPhysicsPhotonsRadiationModels Statisticalbusiness.industryAirRadiotherapy Planning Computer-AssistedReproducibility of ResultsEquipment DesignNeutron radiationEquipment Failure AnalysisIonization chamberBNCTPhysics::Accelerator PhysicsComputer-Aided DesignDose ratebusinessMCNP5Beam (structure)Applied radiation and isotopes : including data, instrumentation and methods for use in agriculture, industry and medicine
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A Monte-Carlo based model of the AX-PET demonstrator and its experimental validation

2013

AX-PET is a novel PET detector based on axially oriented crystals and orthogonal wavelength shifter (WLS) strips, both individually read out by silicon photo-multipliers. Its design decouples sensitivity and spatial resolution, by reducing the parallax error due to the layered arrangement of the crystals. Additionally the granularity of AX-PET enhances the capability to track photons within the detector yielding a large fraction of inter-crystal scatter events. These events, if properly processed, can be included in the reconstruction stage further increasing the sensitivity. Its unique features require dedicated Monte-Carlo simulations, enabling the development of the device, interpreting …

PhotonRadiological and Ultrasound TechnologyPhysics::Instrumentation and Detectors010308 nuclear & particles physicsComputer scienceDetectorMonte Carlo methodWavelength shifter01 natural sciences030218 nuclear medicine & medical imagingComputational science03 medical and health sciences0302 clinical medicinePositron-Emission Tomography0103 physical sciencesRadiology Nuclear Medicine and imagingSensitivity (control systems)ParallaxMonte Carlo MethodImage resolutionSimulationPhysics in Medicine and Biology
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Study of the material of the ATLAS inner detector for Run 2 of the LHC

2017

The ATLAS inner detector comprises three different sub-detectors: the pixel detector, the silicon strip tracker, and the transition-radiation drift-tube tracker. The Insertable B-Layer, a new innermost pixel layer, was installed during the shutdown period in 2014, together with modifications to the layout of the cables and support structures of the existing pixel detector. The material in the inner detector is studied with several methods, using a low-luminosity root s = 13 TeV pp collision sample corresponding to around 2.0 nb(-1) collected in 2015 with the ATLAS experiment at the LHC. In this paper, the material within the innermost barrel region is studied using reconstructed hadronic in…

Photondrift tubePhysics::Instrumentation and Detectors13000 GeV-cmsparticle identification: efficiencyCiencias FísicasPerformance of High Energy Physics Detector01 natural sciencesHigh Energy Physics - Experiment//purl.org/becyt/ford/1 [https]Subatomär fysikHigh Energy Physics - Experiment (hep-ex)Particle tracking detectorsSubatomic Physics[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]scattering [p p]tracking detectorGeneralLiterature_REFERENCE(e.g.dictionariesencyclopediasglossaries)InstrumentationQCMathematical Physicsparticle identification [charged particle]Detector modelling and simulations I (interaction of radiation with matter interaction of photons with matter interaction of hadrons with matter etc)PhysicsLarge Hadron Colliderefficiency [particle identification]track data analysisSettore FIS/01 - Fisica SperimentaleATLAS experimentDetectorpixel [detector]interaction of photons with matterDetectorsMonte Carlo [numerical calculations]ATLASSample (graphics)interaction of hadrons with mattermedicine.anatomical_structureCERN LHC CollLHCcolliding beams [p p]numerical calculations: Monte CarloParticle Physics - ExperimentCIENCIAS NATURALES Y EXACTASp p: scatteringphoton: transition530 PhysicsCiências Naturais::Ciências FísicasInstrumentation:Ciências Físicas [Ciências Naturais]transition [photon]Detector modelling and simulations I (interaction of radiation with matterFOS: Physical sciences610charged particle: particle identificationAccelerator Physics and InstrumentationInteraction of photons with matterOpticsAtlas (anatomy)[ PHYS.HEXP ] Physics [physics]/High Energy Physics - Experiment [hep-ex]0103 physical sciencesmedicinedetector: pixelInteraction of hadrons with matterHigh Energy Physicsddc:610structure010306 general physicsCiencias Exactasetc)Science & TechnologyPixelhep-ex010308 nuclear & particles physicsbusiness.industryinteraction of radiation with matterFísicasiliconAcceleratorfysik och instrumenteringDetector modelling and simulations I (interaction of radiation with matter interaction of photons with matter interaction of hadrons with matter etc); Particle tracking detectors; Performance of High Energy Physics Detectors; Instrumentation; Mathematical Physics//purl.org/becyt/ford/1.3 [https]tracksDetector modelling and simulationsParticle tracking detectorAstronomíarapidityExperimental High Energy PhysicsPerformance of High Energy Physics DetectorsHigh Energy Physics::Experimenttransition radiationbusinessDetector modelling and simulations I (interaction of radiation with matter interaction of photons with matter interaction of hadrons with matter etc)p p: colliding beamsexperimental results
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Phantom size in brachytherapy source dosimetric studies

2004

An important point to consider in a brachytherapy dosimetry study is the phantom size involved in calculations or experimental measurements. As pointed out by Williamson [Med. Phys. 18, 776-786 (1991)] this topic has a relevant influence on final dosimetric results. Presently, one-dimensional (1-D) algorithms and newly-developed 3-D correction algorithms are based on physics data that are obtained under full scatter conditions, i.e., assumed infinite phantom size. One can then assume that reference dose distributions in source dosimetry for photon brachytherapy should use an unbounded phantom size rather than phantom-like dimensions. Our aim in this paper is to study the effect of phantom s…

Photonmedicine.medical_treatmentBrachytherapyMonte Carlo methodBrachytherapyModels BiologicalSensitivity and SpecificityImaging phantomRelative biological effectivenessmedicineHumansScattering RadiationDosimetryComputer SimulationPoint (geometry)RadiometryRadioisotopesPhysicsPhantoms Imagingbusiness.industryRadiotherapy Planning Computer-AssistedReproducibility of ResultsRadiotherapy DosageGeneral MedicineRadiusComputational physicsOrgan SpecificityBody BurdenRadiopharmaceuticalsNuclear medicinebusinessMonte Carlo MethodAlgorithmsRelative Biological EffectivenessMedical Physics
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