Search results for "spectrometer"

showing 10 items of 751 documents

Performance of the NOMAD-STAR detector

2003

The NOMAD-STAR detector is a silicon vertex installed in the NOMAD spectrometer at the CERN SPS neutrino beam. It consists of four layers of a passive boron carbide target with a total mass of 45 kg and five layers of 600 single sided silicon microstrip detectors covering a total area of 1.14m^2. About 11,500 nu_mu charged current interactions were reconstructed in the fiducial volume of NOMAD-STAR from the neutrino run in 1998. The potential use of silicon detectors for nu_mu (nu_e) nu_tau oscillations depends on the observation of the tau candidates by the experimental signature of a large impact parameter, in the case of the one prong decay of the tau, or a double vertex, in the case of …

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderSiliconSpectrometer010308 nuclear & particles physicsPhysics::Instrumentation and DetectorsDetectorFísicachemistry.chemical_elementneutrino physics; silicon microstrip detectors01 natural sciencesNuclear physicschemistry0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]High Energy Physics::ExperimentDetectors and Experimental TechniquesNeutrinoImpact parameter010306 general physicsInstrumentationCharged currentSTAR detector
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Search for νμ(νe) ↔ ντ oscillations with a detector based on a emulsion-silicon target

1996

We discuss the performance of a next generation νμ(νe)↔ ντ oscillation experiment, based on a target consisting of a sandwich of nuclear emulsion layers and silicon detectors. The target would be followed by a full spectrometer for energy-momentum measurement and particle identification. A τ-enriched sample is selected in terms of vertex and kinematical criteria using the electronic spectrometer, with very high efficiency, while at the same time reducing the load of background events to be scanned by up to two orders of magnitude. Events fulfilling the selection criteria are very efficiently located and scanned in the emulsion, thanks to the very good resolution allowed by the silicon track…

PhysicsNuclear and High Energy PhysicsParticle physicsLarge Hadron ColliderSpectrometerPhysics::Instrumentation and DetectorsDetectorMonte Carlo methodParticle identificationNuclear physicsNuclear emulsionDetectors and Experimental TechniquesNeutrino oscillationInstrumentationCharged currentNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Experiments with the High Resolution Kaon Spectrometer at JLab Hall C and the new spectroscopy ofΛ12Bhypernuclei

2014

Since the pioneering experiment E89-009 studying hypernuclear spectroscopy using the (e, e’K+) reaction was completed, two additional experiments, E01-011 and E05-115, were performed at Jefferson Lab. These later experiments used a modified experimental design, the "tilt method", to dramatically suppress the large electromagnetic background, and allowed for a substantial increase in luminosity. Additionally, a new kaon spectrometer, HKS (E01-011), a new electron spectrometer, HES, and a new splitting magnet (E05-115) were added to produce new data sets of precision, high-resolution hypernuclear spectroscopy. All three experiments obtained a spectrum for 12B-Lambda, which is the most charact…

PhysicsNuclear and High Energy PhysicsParticle physicsLuminosity (scattering theory)Electron spectrometerSpectrometer010308 nuclear & particles physicsLambdaHypernucleus01 natural sciencesNuclear physicsMagnet0103 physical sciencesCalibration010306 general physicsSpectroscopyPhysical Review C
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Performance of the photon spectrometer TAPS for deep subthreshold pion detection

2005

Abstract We present in this paper the characteristics of the BaF 2 spectrometer, TAPS, which allow to detect rare electromagnetic events in a high hadronic background. The case of deep subthreshold pions produced in 36 Ar+ 197 Au collisions at 25A and 35A MeV, in which the pion signal is much weaker than the hadronic background and comparable to the cosmic ray background, is studied.

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonSpectrometerSubthreshold conductionNuclear TheoryHadronCosmic raySignalNuclear physicsElectromagnetic calorimeterPionHigh Energy Physics::ExperimentNuclear ExperimentInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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First measurements of Λ and hyperons in elementary electroproduction at MAMI

2010

Abstract Since 2008 the magnetic spectrometer Kaos , dedicated to the detection of charged kaons, is operating at the 1.5 GeV electron beam of MAMI at the Institut fur Kernphysik in Mainz, Germany. The strangeness programme performed in 2008–9 is addressing some important issues in the field of elementary kaon photoelectro-production reactions. The identification of Λ and Σ 0 hyperons in the missing mass spectra from kaon production off a liquid hydrogen target demonstrates the capability of the extended facility to perform strangeness electro-production spectroscopy at low momentum transfers Q 2 0.5 ( GeV / c ) 2 . Systematic uncertainties in the cross-section extraction from the data are …

PhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerField (physics)010308 nuclear & particles physicsNuclear TheoryHyperonStrangeness01 natural sciencesNuclear physicsMomentum0103 physical sciencesMass spectrumHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsSpectroscopyNuclear Physics A
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Studies of high density baryon matter with high intensity heavy-ion beams at J-PARC

2016

Abstract In J-PARC heavy-ion project, we aim at studies of QCD phase structures and hadron properties in high baryon density close to the neutron star core. We have developed a heavy-ion acceleration scheme with a new linac and a new booster with existing two synchrotrons with the goal beam rate of about 10 11 Hz. We have also designed a large acceptance spectrometer based on a toroidal magnet. We have evaluated the spectrometer performance, and demonstrated reconstructing dielectron and dimuon spectra with full detector simulations. Finally, we designed a hypernuclear spectrometer which can utilize the full intensity ion beams.

PhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerIon beam010308 nuclear & particles physicsHadron01 natural sciencesSynchrotronLinear particle acceleratorlaw.inventionBaryonNuclear physicslaw0103 physical sciencesPhysics::Accelerator PhysicsJ-PARCNuclear Experiment010306 general physicsBeam (structure)Nuclear Physics A
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Strange hadronic physics in electroproduction experiments at the Mainz Microtron

2012

Abstract Present and future research into the electroproduction of strangeness plays an important role at Mainz Microtron MAMI. With the Kaos spectrometer for kaon detection operated in the multi-spectrometer facility first cross section measurements of the exclusive p ( e , e ′ K + ) Λ , Σ 0 reactions at low-momentum transfers have been performed. These measurements have clearly discriminated between effective Lagrangian models for photo- and electroproduction of strangeness. Recently, the Kaos spectrometer was upgraded to a double-arm spectrometer for the measurement of elementary cross sections at very forward scattering angles and for the missing mass spectroscopy of hypernuclear states…

PhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerNuclear TheoryHadronStrangeness reactions; Kaon electroproduction; Missing mass spectroscopy; Hypernuclei; Decay-pion spectroscopyStrangenessNuclear physicsCross section (physics)Effective lagrangianNuclear ExperimentSpectroscopyMicrotronBeam (structure)Nuclear Physics A
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Prospects for hypernuclear physics at Mainz: From KAOS@MAMI to PANDA@FAIR

2013

Abstract At the Mainz Microtron hypernuclei are produced by ( e , e ′ K ) reactions. A dedicated kaon spectrometer located at 0° with respect to the electron beam is used to detect kaons emitted in forward direction thus tagging events involving strangeness production. By measuring the momenta of pions from two body weak decays using high resolution magnetic spectrometers one gains direct access to the ground state masses of the produced hyperfragments. At FAIR the PANDA Collaboration intends to produce double-hypernuclei by numbers with an antiproton beam and study their high resolution γ -spectroscopy thus providing for the first time precise information on the level structure of these nu…

PhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerNuclear TheoryStrangeness productionHypernucleusNuclear physicsPionAntiproton beamhypernuclei; weak decay; spectroscopyKAOSGround stateNuclear ExperimentMicrotron
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The Proton Spectrum in Neutron Beta Decay: Latest Results with the aSPECT Spectrometer

2009

Abstract The purpose of the neutron decay spectrometer aSPECT is to determine the antineutrino electron angular correlation coefficient a with high precision. Latest measurements with aSPECT were performed during April/May 2008 at the Institut Laue-Langevin in Grenoble, France. In this paper we give a report on the experiment and the status of the ongoing data analysis.

PhysicsNuclear and High Energy PhysicsParticle physicsSpectrometerProtonCabibbo–Kobayashi–Maskawa matrixSpectrum (functional analysis)ElectronBeta decayPhysics::GeophysicsNuclear physicsAngular correlationNeutronNuclear ExperimentNuclear Physics A
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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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