Search results for "Cherenkov"

showing 10 items of 142 documents

Superbeam studies at CERN

2003

Abstract A conventional low-energy neutrino beam of great intensity could be produced by the Super Proton Linac at CERN as a first stage of a Neutrino Factory. Water Cherenkov and liquid scintillator detectors are studied as possible candidates for a neutrino oscillation experiment which could improve our current knowledge of the atmospheric parameters Δmatm2, θ23 and measure or severely constrain θ13. It is also shown that a very large water detector could eventually observe leptonic CP violation.

PhysicsNuclear and High Energy PhysicsParticle physicsPhysics::Instrumentation and DetectorsHigh Energy Physics::PhenomenologyFísicaSolar neutrino problemAccelerators and Storage RingsNuclear physicsNeutrino detectorCP violationPhysics::Accelerator PhysicsNeutrino FactoryHigh Energy Physics::ExperimentNeutrinoNeutrino oscillationInstrumentationCherenkov radiationLepton
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Measurement of inclusive ρ0, f0(980), f2(1270), K and f′2(1525) production in Z0 decays

1999

DELPHI results are presented on the inclusive production of the neutral mesons ρ0, f0(980), f2(1270), KView the MathML source and f′2(1525) in hadronic Z0 decays. They are based on about 2 million multihadronic events collected in 1994 and 1995, using the particle identification capabilities of the DELPHI Ring Imaging Cherenkov detectors and measured ionization losses in the Time Projection Chamber. The total production rates per hadronic Z0 decay have been determined to be: 1.19±0.10 for ρ0; 0.164±0.021 for f0(980); 0.214±0.038 for f2(1270); 0.073±0.023 for KView the MathML source; and 0.012±0.006 for f′2(1525). The total production rates for all mesons and differential cross-sections for …

PhysicsNuclear and High Energy PhysicsParticle physicsTime projection chamberMeson010308 nuclear & particles physicsElectron–positron annihilationHadron01 natural sciencesParticle identificationIonization0103 physical sciencesLarge Electron–Positron Collider010306 general physicsCherenkov radiationPhysics Letters B
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A luminosity monitor for the A4 parity violation experiment at MAMI

2005

A water Cherenkov luminosity monitor system with associated electronics has been developed for the A4 parity violation experiment at MAMI. The detector system measures the luminosity of the hydrogen target hit by the MAMI electron beam and monitors the stability of the liquid hydrogen target. Both is required for the precise study of the count rate asymmetries in the scattering of longitudinally polarized electrons on unpolarized protons. Any helicity correlated fluctuation of the target density leads to false asymmetries. The performance of the luminosity monitor, investigated in about 2000 hours with electron beam, and the results of its application in the A4 experiment are presented.

PhysicsNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectFOS: Physical sciencesElectronAsymmetryHelicityParticle detectorCharged particleBaryonNuclear physicsHigh Energy Physics::ExperimentNuclear Experiment (nucl-ex)Nuclear ExperimentInstrumentationCherenkov radiationmedia_commonLeptonNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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A simple analytic three-flavour description of the day night effect in the solar neutrino flux

2004

In the 3-flavour framework we derive a simple approximate analytic expression for the day-night difference of the flux of solar $\nu_e$ at terrestrial detectors which is valid for an arbitrary Earth density profile. Our formula has the accuracy of a few per cent and reproduces all the known analytic expressions for the Earth matter effects on the solar neutrino oscillations obtained under simplifying assumptions about the Earth's density profile (matter of constant density, 3 layers of constant densities, and adiabatic approximation). It can also be used for studying the Earth matter effects on the oscillations of supernova neutrinos. We also discuss the possibility of probing the leptonic …

PhysicsNuclear and High Energy PhysicsParticle physicsmedia_common.quotation_subjectSolar neutrinoAstrophysics (astro-ph)FluxFOS: Physical sciencesFísicaAstrophysicsUpper and lower boundsAsymmetryHigh Energy Physics - ExperimentHigh Energy Physics - PhenomenologySupernovaHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Physics::Space PhysicsHigh Energy Physics::ExperimentAstrophysics::Earth and Planetary AstrophysicsNeutrinoCherenkov radiationMixing (physics)media_common
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ALICE T0 detector

2005

T0-the fast timing and trigger detector for the ALICE experiment at CERN LHC-is described. Performance of the T0 prototype measured with a mixture of 6 GeV/c negative pions and kaons is given. The best time resolution (28 ps r.m.s.) was reached with a radiator diameter matching that of the photocathode. The results for all the tested radiator sizes are considerably better than 50 ps-the minimum requirement for the ALICE experiment.

PhysicsNuclear and High Energy PhysicsPhotomultiplierLarge Hadron ColliderPhysics::Instrumentation and DetectorsCherenkov detectorDetectorPhotocathodelaw.inventionNuclear physicsPionNuclear Energy and EngineeringlawRadiator (engine cooling)High Energy Physics::ExperimentElectrical and Electronic EngineeringALICE (propellant)Nuclear ExperimentIEEE Transactions on Nuclear Science
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Prototyping the PANDA Barrel DIRC

2014

The design of the Barrel DIRC detector for the future PANDA experiment at FAIR contains several important improvements compared to the successful BABAR DIRC, such as focusing and fast timing. To test those improvements as well as other design options a prototype was build and successfully tested in 2012 with particle beams at CERN. The prototype comprises a radiator bar, focusing lens, mirror, and a prism shaped expansion volume made of synthetic fused silica. An array of micro-channel plate photomultiplier tubes measures the location and arrival time of the Cherenkov photons with sub-nanosecond resolution. The development of a fast reconstruction algorithm allowed to tune construction deta…

PhysicsNuclear and High Energy PhysicsPhotomultiplierLarge Hadron ColliderPhysics::Instrumentation and Detectorsbusiness.industryDetectorReconstruction algorithmParticle identificationlaw.inventionLens (optics)OpticslawHigh Energy Physics::ExperimentPrismbusinessInstrumentationCherenkov radiationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Recent results with lifetime enhanced microchannel-plate photomultipliers

2018

Abstract The favored photon sensors for the DIRC (detection of internally reflected Cherenkov light) detectors at the PANDA (Anti-proton Annihilation at Darmstadt) experiment at FAIR (Facility for anti-proton and ion research) are micro-channel-plate photomultipliers (MCP-PMTs). The main problem until a few years ago was the limited lifetime of the MCP-PMTs caused by a rapid decrease in quantum efficiency (QE) of the photo cathode (PC) with increasing integrated anode charge (IAC). These limitations are overcome by applying an atomic layer deposition (ALD) coating on the MCPs, as recently done by PHOTONIS and Hamamatsu. During the last years’ tests of lifetime enhanced MCP-PMTs were perform…

PhysicsNuclear and High Energy PhysicsPhotomultiplierPhoton010308 nuclear & particles physicsbusiness.industry01 natural sciencesCathode030218 nuclear medicine & medical imagingAnodelaw.invention03 medical and health sciencesAtomic layer deposition0302 clinical medicineOpticsDetection of internally reflected Cherenkov lightlaw0103 physical sciencesQuantum efficiencyMicrochannel plate detectorbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Investigation of Hamamatsu H8500 phototubes as single photon detectors

2015

We have investigated the response of a significant sample of Hamamatsu H8500 MultiAnode PhotoMultiplier Tubes (MAPMTs) as single photon detectors, in view of their use in a ring imaging Cherenkov counter for the CLAS12 spectrometer at the Thomas Jefferson National Accelerator Facility. For this, a laser working at 407.2 nm wavelength was employed. The sample is divided equally into standard window type, with a spectral response in the visible light region, and UV-enhanced window type MAPMTs. The studies confirm the suitability of these MAPMTs for single photon detection in such a Cherenkov imaging application.

PhysicsNuclear and High Energy PhysicsPhotomultiplierPhotonPhysics - Instrumentation and DetectorsSpectrometerbusiness.industryPhysics::Instrumentation and DetectorsFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)LaserLinear particle acceleratorParticle detectorlaw.inventionOpticslawMeasuring instrumentNuclear Experiment (nucl-ex)businessInstrumentationNuclear ExperimentCherenkov radiation
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The characterisation of the multianode photomultiplier tubes for the RICH-1 upgrade project at COMPASS

2008

Abstract A major upgrade of the Cherenkov photon detection system of COMPASS RICH-1 has been performed and it has been in operation since the 2006 physics run. The inner part of the photon detector has been replaced by a different technology in order to measure Cherenkov photons at high photoelectron rates, up to several times 10 6 per second and per channel. Cherenkov photons from 200 to 750 nm are detected by 576 multianode photomultiplier tubes (MAPMTs) with 16 channels each, coupled to individual fused silica lens telescopes and fast, high sensitivity and high time resolution electronics read-out. To guarantee an optimal performance of the complete system, parameters like dark current, …

PhysicsNuclear and High Energy PhysicsPhotomultiplierPhotonPhysics::Instrumentation and Detectorsbusiness.industryDetectorOpticsUpgradeCompassQuantum efficiencybusinessInstrumentationCherenkov radiationDark current
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High Precision Momentum Calibration of the Magnetic Spectrometers at MAMI for Hypernuclear Binding Energy Determination

2016

We propose a new method for absolute momentum calibration of magnetic spectrometers used in nuclear physics, using the time-of-flight (TOF), differences of pairs of particles with different masses. In cases where the flight path is not known, a calibration can be determined by using the TOF differences of two pair combinations of three particles. A Cherenkov detector, read out by a radio frequency photomultiplier tube, is considered as the high-resolution and highly stable TOF detector. By means of Monte Carlo simulations it is demonstrated that the magnetic spectrometers at the MAMI electron-scattering facility can be calibrated absolutely with an accuracy $\delta p/p\leq 10^{-4}$, which w…

PhysicsNuclear and High Energy PhysicsPhotomultiplierPhysics - Instrumentation and DetectorsSpectrometer010308 nuclear & particles physicsCherenkov detectorPhysics::Instrumentation and DetectorsMonte Carlo methodDetectorFOS: Physical sciencesInstrumentation and Detectors (physics.ins-det)01 natural scienceslaw.inventionMomentumNuclear physicsTime of flightlaw0103 physical sciencesCalibrationNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentInstrumentationNuclear Experiment
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