Search results for " Scintillators"

showing 10 items of 20 documents

Exciton interaction with Ce3+ and Ce4+ ions in (LuGd)3(Ga,Al)5O12 ceramics

2021

The authors acknowledge the expert help of the staff of MAX IV Laboratory. The research leading to this result has been supported by the project CALIPSOplus under the Grant Agreement 730872 from the EU Framework Programme for Research and Innovation HORIZON 2020. I.V. acknowledges the support of Russian Foundation for Basic Research # 20-52-S52001.

Materials scienceAbsorption spectroscopyExcitonBiophysicsAnalytical chemistry02 engineering and technology010402 general chemistry01 natural sciences7. Clean energyBiochemistryCeSynchrotronTheoryofComputation_ANALYSISOFALGORITHMSANDPROBLEMCOMPLEXITYSpectroscopy:NATURAL SCIENCES::Physics [Research Subject Categories]General Chemistry021001 nanoscience & nanotechnologyCondensed Matter PhysicsAtomic and Molecular Physics and OpticsXANESXANES0104 chemical sciencesAbsorption edgeCe4+Absorption bandEnergy transferGarnet scintillatorsExcited stateExcitons0210 nano-technologyLuminescence
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SiPMs coated with TPB: coating protocol and characterization for NEXT

2012

[EN] Silicon photomultipliers (SiPM) are the photon detectors chosen for the tracking readout in NEXT, a neutrinoless \bb decay experiment which uses a high pressure gaseous xenon time projection chamber (TPC). The reconstruction of event track and topology in this gaseous detector is a key handle for background rejection. Among the commercially available sensors that can be used for tracking, SiPMs offer important advantages, mainly high gain, ruggedness, cost-effectiveness and radio-purity. Their main drawback, however, is their non sensitivity in the emission spectrum of the xenon scintillation (peak at 175 nm). This is overcome by coating these sensors with the organic wavelength shifte…

Materials sciencePhysics - Instrumentation and DetectorsFOS: Physical scienceschemistry.chemical_elementengineering.materialWavelength shifterTracking (particle physics)7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentTECNOLOGIA ELECTRONICAHigh Energy Physics - Experiment (hep-ex)XenonSilicon photomultiplierCoating0103 physical sciencesSensitivity (control systems)Visible and IR photons (solid-state)010306 general physicsInstrumentationPhoton detectors for UVMathematical PhysicsScintillationTime projection chamber010308 nuclear & particles physicsbusiness.industryTime projection Chambers (TPC)FísicaDetectorsInstrumentation and Detectors (physics.ins-det)Gas detectorsScintillators scintillation and light emission processes (solid gas and liquid scintillators)Detectors de gasoschemistryParticle tracking detectors (Solid-state detectors)engineeringOptoelectronicsbusiness
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Prompt Photon Identification in the ALICE Experiment: The Isolation Cut Method

2007

Submitted for publication in NIM; The ALICE experiment at LHC will detect and identify prompt photons and light neutral mesons with the PHOS and EMCal detectors. Charged particles will be detected and identified by the central tracking system. In this paper, a method to identify prompt photons and to separate them from the background of hadrons and decay photons in PHOS with the help of isolation cuts is presented.

Nuclear and High Energy PhysicsParticle physicsPhotonelectromagnetic calorimetersMesonquark-gluon plasmaPhysics::Instrumentation and DetectorsHadronPhysics::OpticsParton25.75.Nq 24.10.Lx 25.75.-q 29.40.Vj[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencesNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]PWO scintillators010306 general physicsNuclear ExperimentInstrumentationPhysicsLarge Hadron Collider010308 nuclear & particles physicsHigh-energy gamma raysCharged particleQuark–gluon plasmaHigh Energy Physics::ExperimentALICE (propellant)
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Spectral modeling of scintillator for the NEMO-3 and SuperNEMO detectors

2010

We have constructed a GEANT4-based detailed software model of photon transport in plastic scintillator blocks and have used it to study the NEMO-3 and SuperNEMO calorimeters employed in experiments designed to search for neutrinoless double beta decay. We compare our simulations to measurements using conversion electrons from a calibration source of $\rm ^{207}Bi$ and show that the agreement is improved if wavelength-dependent properties of the calorimeter are taken into account. In this article, we briefly describe our modeling approach and results of our studies.

Nuclear and High Energy PhysicsPhotomultiplierTechnologyPhysics - Instrumentation and DetectorsPhotonPhysics::Instrumentation and DetectorsCODEFOS: Physical sciencesScintillator01 natural sciencesHigh Energy Physics - ExperimentPhysics Particles & FieldsNuclear physicsHigh Energy Physics - Experiment (hep-ex)Photomultiplier0202 Atomic Molecular Nuclear Particle And Plasma PhysicsDouble beta decay0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]CalibrationPlastic scintillators[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]010306 general physicsNuclear Science & TechnologyInstrumentationInstruments & InstrumentationScintillationphysics.ins-detPhysicsScintillationScience & Technology010308 nuclear & particles physicshep-exPhysicsMO-100DetectorInstrumentation and Detectors (physics.ins-det)Double beta decayNuclear & Particles PhysicsCalorimeterPhysics NuclearPhysical SciencesGEANT 4DOUBLE-BETA DECAYOptical photon transport
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Detection of charged pions and protons in the segmented electromagnetic calorimeter TAPS

1998

We present the characteristics of the segmented BaF2 calorimeter TAPS for the measurement of charged pions and protons. The method of particle identification exploits the relation between the kinetic energy of a particle, its mass and the time-of-flight required to reach the detector. The detection efficiency is calculated using GEANT-GCALOR simulations. The analysis method is applied in the reaction Ar-40 + Ca-nat at 0.8A GeV. The simultaneous detection of charged pions and protons can be used to search for correlated pairs signalling the de-excitation of the Delta(1232) resonance. (C) 1998 Elsevier Science B.V. All rights reserved.

Nuclear and High Energy PhysicsPhotonBAF2 SCINTILLATORSHEAVY-ION COLLISIONSPHOTONSKinetic energy01 natural sciencesResonance (particle physics)Particle identificationENERGYNuclear physicsPion0103 physical sciencesABSORPTIONPARTICLESNuclear Experiment010306 general physicsInstrumentationcharged pion detectionPhysicsDelta(1232) resonance detectionCalorimeter (particle physics)010308 nuclear & particles physicsDetectorproton detection[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]ParticleHigh Energy Physics::ExperimentAtomic physics
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Characterization of a cylindrical plastic {\beta}-detector with Monte Carlo simulations of optical photons

2017

V. Guadilla et al. -- 5 pags., 8 figs., tab.

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsPhotonTotal absorption spectroscopyoptical photonsTotal absorption spectroscopyMonte Carlo method[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]7. Clean energy01 natural sciencesElectromagnetic radiationMonte Carlo simulationsOptics0103 physical sciencesPlastic scintillators[PHYS.PHYS.PHYS-INS-DET]Physics [physics]/Physics [physics]/Instrumentation and Detectors [physics.ins-det]plastic scintillators010306 general physicsAbsorption (electromagnetic radiation)Nuclear ExperimentInstrumentationPhysicsSpectrometerta114010308 nuclear & particles physicsbusiness.industryDetectortotal absorption spectroscopyComputational physicsOptical photonsDynamic Monte Carlo methodbusiness
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Mitigation of backgrounds from cosmogenic 137 Xe in xenon gas experiments using 3 He neutron capture

2020

[EN] Xe-136 is used as the target medium for many experiments searching for 0 nu beta beta. Despite underground operation, cosmic muons that reach the laboratory can produce spallation neutrons causing activation of detector materials. A potential background that is difficult to veto using muon tagging comes in the form of Xe-137 created by the capture of neutrons on Xe-136. This isotope decays via beta decay with a half-life of 3.8 min and a Q(beta) of similar to 4.16 MeV. This work proposes and explores the concept of adding a small percentage of He-3 to xenon as a means to capture thermal neutrons and reduce the number of activations in the detector volume. When using this technique we f…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsScintillation and light emission processesGas and liquid scintillatorsFOS: Physical scienceschemistry.chemical_element01 natural sciences7. Clean energyHigh Energy Physics - ExperimentTECNOLOGIA ELECTRONICANuclear physicsGaseous detectorsSolidHigh Energy Physics - Experiment (hep-ex)XenonDouble beta decay0103 physical sciencesIsotopes of xenonSpallationNeutron010306 general physicsPhysics010308 nuclear & particles physicsFísicaInstrumentation and Detectors (physics.ins-det)Beta DecayNeutron temperatureNeutron capturechemistryScintillatorsRadioactive decayJournal of Physics G: Nuclear and Particle Physics
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Probing the Merits of Different Event Parameters for the Identification of Light Charged Particles in CHIMERA CsI(Tl Detectors With Digital Pulse Sha…

2013

We investigated the merits of different event parameters in the identification of Light Charged Particles (LCPs) with CsI(Tl) scintillators read out by photodiodes at high incident energy (400 MeV/u). This investigation is made possible by digital signal processing the output signals. As in the conventional analogue case, the digitized signals allow the discrimination of light charged particles by computing the fast and slow components. In addition other identification parameters as the rise time of the output pulses of the CsI(Tl) come out nearly for free. Aim of this paper is the investigation of novel identification plots and the probe of their merits, in particular at relativistic energ…

Nuclear and High Energy PhysicsPhysics::Instrumentation and Detectorsintermediate energy nuclear physicpulse shape analysiScintillatorParticle identificationlaw.inventionOpticslawElectrical and Electronic EngineeringDigital signal processingPhysicsonline digital signal processingSignal processingsezeleCsI(Tl) scintillatorsbusiness.industrypulse shape analysisDetectorCsI(Tl) scintillatorCsI(Tl) scintillators; intermediate energy nuclear physics; online digital signal processing; particle identification; pulse shape analysisCsI(Tl) scintillators; intermediate energy nuclear physics; online digital signal processing; particle identification; pulse shape analysis; Electrical and Electronic Engineering; Nuclear Energy and Engineering; Nuclear and High Energy PhysicsCharged particlePhotodiodeintermediate energy nuclear physicsNuclear Energy and EngineeringRise timeparticle identificationbusinessnuclear physics; heavy-ions; digital signal processing; scintillation detectors
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On the performances of a particle tracking detector based on triangular scintillator bars read out by silicon photomultipliers

2020

Abstract A tracking detector composed of scintillator bars with a triangular cross-section read out by silicon photomultipliers in analog mode was developed. The tracker was designed to instrument a low density spectrometer for neutrino experiments. The performance of the system has been studied by exposing it to charged particle beams at the CERN-PS. The tests have shown that the position resolution in reconstructing charged particles’ tracks is within 2.2 mm over the momentum range 0.5–10 GeV/c.

Nuclear and High Energy PhysicsScintillators SiPM Particle tracking device Position resolutionParticle tracking devicePhysics::Instrumentation and DetectorsSiPMScintillatorTracking (particle physics)01 natural sciences030218 nuclear medicine & medical imaging03 medical and health sciences0302 clinical medicineOpticsSilicon photomultiplierParticle tracking device Position resolution Scintillators SiPM0103 physical sciencesInstrumentationPhysicsRange (particle radiation)Spectrometer010308 nuclear & particles physicsbusiness.industrySettore FIS/01 - Fisica SperimentaleDetectorCharged particleScintillatorsPosition resolutionHigh Energy Physics::ExperimentNeutrinobusiness
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Charge reconstruction in large-area photomultipliers

2018

Large-area PhotoMultiplier Tubes (PMT) allow to efficiently instrument Liquid Scintillator (LS) neutrino detectors, where large target masses are pivotal to compensate for neutrinos' extremely elusive nature. Depending on the detector light yield, several scintillation photons stemming from the same neutrino interaction are likely to hit a single PMT in a few tens/hundreds of nanoseconds, resulting in several photoelectrons (PEs) to pile-up at the PMT anode. In such scenario, the signal generated by each PE is entangled to the others, and an accurate PMT charge reconstruction becomes challenging. This manuscript describes an experimental method able to address the PMT charge reconstruction …

PhotomultiplierLiquid detectorsvisible and IR photons (vacuum) (photomultipliers HPDs others)Physics - Instrumentation and Detectorsgas and liquid scintillators)Physics::Instrumentation and DetectorsPhoton detectors for UV visible and IR photons (vacuum) (photomultipliers HPDs others)FOS: Physical sciencesvisible and IR photons (vacuum) (photomultipliers HPDsScintillatorvisible and IR photons (vacuum) (photomultipliers01 natural sciencesParticle detectorNOsymbols.namesakeOptics0103 physical sciencesCalorimeter methods010306 general physicsInstrumentationPhoton detectors for UVMathematical PhysicsPhysicsscintillation and light emission processes (solid gas and liquid scintillators)010308 nuclear & particles physicsbusiness.industrySettore FIS/01 - Fisica SperimentaleWiener filterDetectorReconstruction algorithmScintillators scintillation and light emission processes (solid gas and liquid scintillators)Instrumentation and Detectors (physics.ins-det)Scintillatorscintillation and light emission processes (solidCalorimeter methods; Liquid detectors; Photon detectors for UV visible and IR photons (vacuum) (photomultipliers HPDs others); Scintillators scintillation and light emission processes (solid gas and liquid scintillators)Photon detectors for UV visible and IR photons (vacuum) (photomultipliers HPDs others)Neutrino detectorHPDsCalorimeter methodScintillatorsScintillators scintillation and light emission processes (solid gas and liquid scintillators)symbolsLiquid detectorCalorimeter methods; Liquid detectors; Photon detectors for UV visible and IR photons (vacuum) (photomultipliers HPDs others); Scintillators scintillation and light emission processes (solid gas and liquid scintillators)Deconvolutionbusinessothers)scintillation and light emission processes (solid gas and liquid scintillators)
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