Search results for "light"

showing 10 items of 3575 documents

The PANDA DIRC detectors

2020

Abstract The PANDA experiment at the future Facility for Antiproton and Ion Research (FAIR) will address fundamental questions of hadron physics with unprecedented precision. To reach this goal excellent Particle Identification (PID) is essential over a large range of particle momenta and solid angles. Most of the phase space will be covered by two innovative DIRC (Detection of Internally Reflected Cherenkov light) detectors. The Endcap Disc DIRC and Barrel DIRC will cover the polar angle range from 5 to 22°and 22 to 140°, respectively. Both detectors rely on high precision optical components, lifetime-enhanced Microchannel Plate PMTs (MCP-PMTs), and fast readout electronics.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Physics::Instrumentation and Detectors010308 nuclear & particles physicsCherenkov detectorbusiness.industryDetectorSolid angle01 natural sciencesParticle identificationlaw.inventionOpticslawDetection of internally reflected Cherenkov light0103 physical sciencesFacility for Antiproton and Ion ResearchHigh Energy Physics::ExperimentMicrochannel plate detector010306 general physicsbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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A novel method for obtaining continuous stopping power curves

2001

Abstract A new method has been developed for obtaining continuous stopping power curves in transmission geometry. In the method both the incident energy of the particle and its energy after passing through the sample foil are extracted directly from the semiconductor detector. Full range of energies is measured simultaneously eliminating step-by-step measurements and providing continuous data. A time-of-flight (TOF) spectrometer provides unambiguous matching of relevant particle groups from the run with and without absorber. Suitable energy distribution of incident particles was achieved by choosing the right thickness and tilting angle of a scattering foil. The method is very fast and reli…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Spectrometerbusiness.industrySemiconductor detectorTime of flightOpticsCalibrationStopping power (particle radiation)Specific energybusinessInstrumentationEnergy (signal processing)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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A highly-segmented ΔE-time-of-flight wall as forward detector of the 4π-system for charged particles at the SIS/ESR accelerator

1993

Abstract At the SIS/ESR accelerator facility at GSI in Darmstadt the 4π-detector system FOPI is under construction at present. It is designed for the investigation of central collisions of heavy ions in the energy range up to 2 A GeV. As phase I of this detector a forward wall has been built and used in various experiments. It comprizes a total number of 764 scintillators with an additional shell of 188 thin ΔE -detectors in front of it and covers the full azimuth of the polar angles from 1° to 30°. The velocity and the nuclear charge of the fragments are determined by a combined time-of-flight and ΔE measurement.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Wire chamberPhysics::Instrumentation and DetectorsNuclear TheoryDetectorScintillatorParticle detectorCharged particleNuclear physicsTime of flightIonization chamberAtomic physicsNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Effects of scintillation light collection on the time resolution of a time-of-flight detector for annihilation quanta

1990

Monte Carlo methods were used to simulate the production and collection of scintillation light in a BaF/sub 2/ crystal. The calculated results were compared to measured values for detectors with different heights. Based on this simulation, a TOF (time-of-flight) detector consisting of two conical BaF/sub 2/ crystals (base radius 18 mm, top radius 15 mm, height 25 mm) was assembled. The total time resolution of this system was (210+or-5) ps FWHM (full width at half maximum) for 511-keV annihilation quanta and was found to be independent of the source position between the detectors. Since the time resolution of the TOF detector system consisting of two conical BaF/sub 2/ crystals is sufficien…

PhysicsNuclear and High Energy PhysicsScintillationAnnihilationTime of flight detectorPhysics::Instrumentation and Detectorsbusiness.industryDetectorMonte Carlo methodRadiusNuclear physicsFull width at half maximumOpticsNuclear Energy and EngineeringScintillation counterElectrical and Electronic EngineeringbusinessIEEE Transactions on Nuclear Science
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Digital pulse-shape analysis with a TRACE early silicon prototype

2014

[EN] A highly segmented silicon-pad detector prototype has been tested to explore the performance of the digital pulse shape analysis in the discrimination of the particles reaching the silicon detector. For the first time a 200 tun thin silicon detector, grown using an ordinary floating zone technique, has been shown to exhibit a level discrimination thanks to the fine segmentation. Light-charged particles down to few MeV have been separated, including their punch-through. A coaxial HPGe detector in time coincidence has further confirmed the quality of the particle discrimination. K.; 2014 Elsevier B.V. All rights reserved

PhysicsNuclear and High Energy PhysicsSilicon detectorSiliconPhysics::Instrumentation and Detectorsbusiness.industryLight-charged particlesDetectorchemistry.chemical_element[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]Particle detectorParticle identificationSemiconductor detectorParticle identificationTECNOLOGIA ELECTRONICAOpticschemistryMeasuring instrumentGamma-ray spectroscopyCoaxialbusinessDigital pulse shape analysisInstrumentationElectronic circuit
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The ISOLDE Silicon Ball

2003

The development of new spectroscopy devices with the capability of detecting charged particles and precisely determining their energy, angular distribution and nature has become one of the requirements for the investigation of weakly bound nuclei close to the particle driplines. With this aim the ISOLDE Silicon Ball is under construction. It is a charged particle spectroscopy device allowing for the investigation of the exotic nuclei produced at ISOLDE and at other similar facilities. Very high geometrical efficiency and broad energy range coverage are required. In order to allow for particle identification the simultaneous use of the Time of Flight and Pulse Shape Discrimination techniques…

PhysicsNuclear and High Energy PhysicsSilicon010308 nuclear & particles physicschemistry.chemical_element7. Clean energy01 natural sciencesParticle identificationCharged particleNuclear physicsTime of flightAngular distributionRecoilchemistry0103 physical sciencesBall (bearing)Physics::Accelerator PhysicsNuclear Experiment010306 general physicsSpectroscopyInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Experimental Linear Energy Transfer of Heavy Ions in Silicon for RADEF Cocktail Species

2009

Experimental linear energy transfer values of heavy ions in silicon are presented with comparison to estimations from different semi empirical codes widely used among the community. This paper completes the experimental LET data for the RADEF cocktail ions in silicon.

PhysicsNuclear and High Energy PhysicsSiliconLinear energy transferchemistry.chemical_elementProbability density functionIonNuclear physicsTime of flightNuclear Energy and EngineeringIon acceleratorschemistryElectrical and Electronic EngineeringAtomic physicsNuclear ExperimentIEEE Transactions on Nuclear Science
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Particle identification with time-of-flight and pulse-shape discrimination in neutron-transmutation-doped silicon detectors

2009

Abstract A method for the identification of energetic charged particles has been investigated based on the employment of pulse-shape discrimination (PSD) in a silicon detector in addition to conventional time-of-flight (ToF) techniques. The method makes use of the fact that, at fixed energy, the particle's velocity, or ToF, is a measure of the particle's mass A while the time structure of the current pulse in a silicon energy detector, used as the ToF stop, permits identification of nuclear charges Z. In the measurements presented here, ToF and PSD methods were applied simultaneously. We used micro-channel plate (MCP) detectors as fast time pick-offs and surface-barrier (SB) n-type Si detec…

PhysicsNuclear and High Energy PhysicsSiliconPhysics::Instrumentation and DetectorsPreamplifierbusiness.industryDetectorchemistry.chemical_elementParticle detectorCharged particleParticle identificationNuclear physicsTime of flightOpticschemistryNeutronbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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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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Time response of TOF spectrometer to light and heavy particles

2002

Comparing time of flight (TOF) values for α particles and fission fragments measured at different distances between the start- and stop detector we have obtained 60 ps as the upper limit for the TOF error resulting from the assumption of equal and linear time calibrations for both types of particles. While the 60 ps limit relates only to the specific spectrometer, the problem and the suggested verification technique are of general interest.

PhysicsNuclear and High Energy PhysicsSpectrometerPhysics::Instrumentation and DetectorsFissionDetectorAnalytical chemistryAlpha particleTime of flightTime responseMicrochannel plate detectorLimit (mathematics)Nuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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