Search results for "Microtron"

showing 10 items of 149 documents

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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Characterisation and calibration of a scintillating fibre detector with > 4000 multi-anode photomultiplier channels

2012

In the Kaos spectrometer at the Mainz Microtron a high-resolution coordinate detector for high-energy particles is operated. It consists of scintillating fibres with diameters of 4000 multi-anode photomultiplier channels. It is one of the most modern focal-plane detectors for magnetic spectrometers world-wide. To correct variations in the detection efficiency, caused by the different gains and the different optical transmittances, a fully automated off-line calibration procedure has been developed. The process includes the positioning of a radioisotope source alongside the detector plane and the automated acquisition and analysis of the detector signals. It was possible to characterise and …

PhysicsNuclear and High Energy PhysicsPhotomultiplierPhysics - Instrumentation and DetectorsSpectrometerbusiness.industryPhysics::Instrumentation and DetectorsDetectorAnodeFibre ChannelOpticsCalibrationScintillating fibrebusinessNuclear ExperimentInstrumentationMicrotron
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Noise and radiation damage in silicon photomultipliers exposed to electromagnetic and hadronic radiation

2009

For the electron arm tracking system in the KAOS spectrometer at the Mainz Microtron MAMI a detector based on 2 m long scintillating fibres read out by silicon photomultipliers (SiPM) is planned. Because of the detector's close proximity to the intense electron beam a study of noise and radiation damage in SiPM has been performed. A sample of devices was exposed directly to a 14 MeV electron beam and to a mixed radiation field in the experimental area. First noticeable effects are a large increase in the dark count rate and a severe loss of the gain uniformity.

PhysicsNuclear and High Energy PhysicsPhotomultiplierPhysics::Instrumentation and Detectorsbusiness.industryRadiationParticle detectorOpticsSilicon photomultiplierElectron beam processingRadiation damageNuclear ExperimentbusinessInstrumentationMicrotronNoise (radio)Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Front-End Electronics for the KAOS Spectrometer at MAMI

2009

A new front-end electronics system has been developed for the electron arm tracking detectors in the Kaos spectrometer at the Mainz microtron MAMI. The signals of multi-anode photomultipliers are collected by 96-channel front-end boards, digitized by double-threshold discriminators and the signal time is picked up by F1 TDC chips. The system was designed to process more than 4,000 channels and to cope with the high electron flux in the spectrometer and the high count rate requirement of the detectors. A subset of 288 channels was installed and successfully used in the 2008 data taking period of the Kaos spectrometer.

PhysicsNuclear and High Energy PhysicsPhotomultiplierSpectrometerbusiness.industryDetectorElectrical engineeringTracking (particle physics)Signaldouble-threshold discriminator; front-end electronics; multi-anode photomultiplier; microtronNuclear Energy and EngineeringNuclear electronicsElectrical and Electronic EngineeringKAOSbusinessMicrotronIEEE Transactions on Nuclear Science
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In-beam tests of scintillating fibre detectors at MAMI and at GSI

2008

The performance of scintillating fibre detectors was studied with electrons at the spectrometer facility of the Mainz microtron MAMI, as well as in a C-12 beam of 2 AGeV energy and in a beam of different particle species at GSI. Multi-anode photomultipliers were used to read out one or more bundles of 128 fibres each in different geometries. For electrons a time resolution of FWHM = 1 ns was measured in a single detector plane with a detection efficiency epsilon > 99%. A time resolution of 310 ps (FWHM) between two planes of fibres was achieved for carbon ions, leading to a FWHM = 220 ps for a single detector. The hit position residual was measured with a width of FWHM = 0.27 mm. The var…

PhysicsNuclear and High Energy PhysicsPhotomultiplierSpectrometerbusiness.industryDetectorFOS: Physical sciencesCharged particleParticle detectorNuclear physicsFull width at half maximumOpticsNuclear Experiment (nucl-ex)businessInstrumentationMicrotronNuclear ExperimentBeam (structure)
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Threshold π0 photoproduction on transverse polarised protons at MAMI

2015

Abstract Polarisation-dependent differential cross sections σ T associated with the target asymmetry T have been measured for the reaction γ p → → p π 0 with transverse target polarisation from π 0 threshold to photon energies of 190 MeV. The data were obtained using a frozen-spin butanol target with the Crystal Ball / TAPS detector set-up and the Glasgow photon tagging system at the Mainz Microtron MAMI. Results for σ T have been used in combination with our previous measurements of the unpolarised cross section σ 0 and the beam asymmetry Σ for a model-independent determination of S- and P-wave multipoles in the π 0 threshold region, which includes for the first time a direct determination…

PhysicsNuclear and High Energy PhysicsPhotonChiral perturbation theoryScatteringmedia_common.quotation_subjectAsymmetryNuclear physicsCross section (physics)Transverse planeAtomic physicsNuclear ExperimentMultipole expansionMicrotronmedia_commonPhysics Letters B
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The angular distribution of the 12C(γ,pn) reaction for Eγ=120−150 MeV

1998

The angular distribution of nucleons emitted in the 12C(γ,pn) reaction has been measured using tagged photons at the Mainz microtron MAMI. The variation of the reaction strength with the polar angles of the two emitted nucleons is reported for Eγ=120−150 MeV. The proton angular distribution peaks at more backward angles than the 2H(γ,p) differential cross section indicating a departure from the simple quasi-deuteron model of 2N photo-emission. The distribution shape is in reasonable agreement with microscopic theoretical models which include both π- and ρ-exchange.

PhysicsNuclear and High Energy PhysicsPhotonProtonNuclear TheoryShape of the distributionNuclear physicsAngular distributionNuclear fusionPolarAtomic physicsNuclear ExperimentNucleonMicrotronThe European Physical Journal A
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Channeling experiments with sub-GeV electrons in flat silicon single crystals

2015

Abstract Various planar channeling experiments, performed at the Mainz Microtron MAMI with electrons at silicon single crystals, have been reanalyzed. Two types of signals have been employed. The low energy loss signal originates from emission of channeling radiation in the energy domain between 0.4 and 9 MeV while the high energy loss signal from electrons which have lost about 50% of their primary energy by emission of bremsstrahlung photons. The (1 1 0) planar channeling data, taken at a beam energy of 855 MeV with the former signal, can well be described on the basis of the solution of the classical Fokker–Planck equation. The measurements with the latter signal at beam energies between…

PhysicsNuclear and High Energy PhysicsPhotonSiliconBremsstrahlungchemistry.chemical_elementElectronRadiationCrystalchemistryAtomic physicsNuclear ExperimentInstrumentationMicrotronBeam (structure)Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms
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Measurement of theγp→K0Σ+reaction with the Crystal Ball/TAPS detectors at the Mainz Microtron

2013

The gamma p -> K-0 Sigma(+) reaction has been measured from threshold to E-gamma = 1.45 GeV (W-CM = 1.9 GeV) using the Crystal Ball and TAPS multiphoton spectrometers together with the photon tagging facility at the Mainz Microtron MAMI. In the present experiment, this reaction was searched for in the 3 pi(0)p final state, by assuming K-S(0) -> pi(0)pi(0) and Sigma(+) -> pi(0)p. The experimental results include total and differential cross sections as well as the polarization of the recoil hyperon. The new data significantly improve empirical knowledge about the gamma p -> K-0 Sigma(+) reaction in the measured energy range. The results are compared to previous measurements and model predict…

PhysicsNuclear and High Energy PhysicsPhotonSpectrometerProton010308 nuclear & particles physicsHyperonSigma01 natural sciencesNuclear physicsRecoil0103 physical sciences010306 general physicsMicrotronCrystal BallPhysical Review C
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Novel optical interferometry of synchrotron radiation for absolute electron beam energy measurements

2018

Abstract A novel interferometric method is presented for the measurement of the absolute energy of electron beams. In the year 2016, a pioneering experiment was performed using a 195 MeV beam of the Mainz Microtron (MAMI). The experimental setup consisted of two collinear magnetic undulators as sources of coherent optical synchrotron light and a high-resolving grating monochromator. Beam energy measurements required the variation of the relative undulator distance in the decimeter range and the analysis of the intensity oscillation length in the interference spectrum. A statistical precision of 1 keV was achieved in 1 h of data taking, while systematic uncertainties of 700 keV were present …

PhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsSpectrometer010308 nuclear & particles physicsbusiness.industrySynchrotron radiationFOS: Physical sciencesParticle acceleratorInstrumentation and Detectors (physics.ins-det)Undulator01 natural sciencesSynchrotronlaw.inventionOpticslaw0103 physical sciencesPhysics::Accelerator Physics010306 general physicsbusinessNuclear ExperimentInstrumentationMicrotronBeam (structure)Monochromator
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