Search results for "Microtron"

showing 10 items of 149 documents

Future use of silicon photomultipliers for Kaos at MAMI and P¯ANDA at FAIR

2009

A characterisation of scintillating fibres with silicon photomultiplier read-out was performed in view of their possible application in fibre tracking detector systems. Such a concept is being considered for the Kaos spectrometer at the Mainz Microtron MAMI and as a time-of-flight start detector for the hypernuclear physics programme at the PANDA experiment of the FAIR project. Results on particle detection effciency and time resolution are discussed. In summary, the silicon devices are very suitable for the detection of the low light yield from scintillating fibres insofar a trigger scheme is found to cope with the noise rate characteristics.

Fibre trackingPhysicsNuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsSiliconSpectrometerPhysics::Instrumentation and Detectorsbusiness.industryDetectorFOS: Physical scienceschemistry.chemical_elementTime resolutionInstrumentation and Detectors (physics.ins-det)OpticsSilicon photomultiplierchemistryNuclear Experiment (nucl-ex)KAOSNuclear ExperimentbusinessNuclear ExperimentInstrumentationMicrotronNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Application of 61Ni Mössbauer spectroscopy to chemical problems

1996

Using the possibility to produce 61Co sources at the MAinz MIcrotron, 61Ni Mossbauer spectroscopy was applied to different kinds of chemical problems. Measurements of isomer shifts and V zz values in some common compounds and compounds with unusual chemical bonding for comparison with band structure calculations, measurement of 61Ni Mossbauer parameters in model compounds for hydrogenase and dehydrogenase with an active [NiS4] centre, and study of novel binary NiF3 compounds at helium temperature are presented.

HydrogenaseMaterials scienceNuclear magnetic resonanceChemical bondMössbauer spectroscopyGeneral Physics and AstronomyPhysical chemistryMossbauer spectraElectronic band structureMicrotronHelium temperatureIl Nuovo Cimento D
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Experimental investigations of the hypernucleus $_Λ^4$H

2015

International audience; Negatively charged pions from two-body decays of stopped _Lambda^4H hypernuclei were studied in 2012 at the Mainz Microtron MAMI, Germany. The momenta of the decay-pions were measured with unprecedented precision by using high-resolution magnetic spectrometers. A challenge of the experiment was the tagging of kaons from associated K^+∧ production off a Be target at very forward angles. In the year 2014, this experiment was continued with a better control of the systematic uncertainties, with better suppression of coincident and random background, improved particle identification, and with higher luminosities. Another key point of the progress was the improvemen…

Lambda: hypernucleusQC1-999Nuclear TheoryAstrophysics[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]01 natural sciencestagged beamParticle identificationpi-010305 fluids & plasmasNuclear physicsMomentumMainz LinacPionCoincidentberyllium: target0103 physical sciencesCalibration010306 general physicsNuclear ExperimentMicrotronPhysicsSpectrometerPhysicspi: decayresolutionsuppressionHypernucleusmagnetic spectrometerKmicrotronhydrogenmomentum: calibrationbackground: randomHigh Energy Physics::Experimentluminosity: highparticle identification
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Measurement of the Generalized Polarizabilities of the Proton at Intermediate $Q^2$

2021

Background: Generalized polarizabilities (GPs) are important observables to describe the nucleon structure, and measurements of these observables are still scarce. Purpose: This paper presents details of a virtual Compton scattering (VCS) experiment, performed at the A1 setup at the Mainz Microtron by studying the $e p \to e p \gamma$ reaction. The article focuses on selected aspects of the analysis. Method: The experiment extracted the $P_{LL} -P_{TT} / \epsilon$ and $P_{LT}$ structure functions, as well as the electric and magnetic GPs of the proton, at three new values of the four-momentum transfer squared $Q^2$: 0.10, 0.20 and 0.45 GeV$^2$. Results: We emphasize the importance of the ca…

MAINZ-A1ProtonNuclear Theory[PHYS.NUCL]Physics [physics]/Nuclear Theory [nucl-th]higher-orderHadronic Physics and QCDFOS: Physical sciences[PHYS.NEXP]Physics [physics]/Nuclear Experiment [nucl-ex]momentum transfer dependence01 natural scienceselectron p: scatteringNuclear Theory (nucl-th)Cross section (physics)High Energy Physics - Phenomenology (hep-ph)Polarizability0103 physical sciencesCalibrationp: structure functionNuclear Experiment (nucl-ex)010306 general physicsMicrotronNuclear ExperimentPhysics010308 nuclear & particles physicsCompton scatteringObservablecross section: measuredcalibrationComputational physicsHigh Energy Physics - Phenomenology[PHYS.HPHE]Physics [physics]/High Energy Physics - Phenomenology [hep-ph]p: polarizabilityelectron p --> electron p photonNucleonCompton scatteringexperimental results
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Photoemission of spinpolarized electrons from strained GaAsP

1996

Strained layer GaAs.95P.05 photo cathodes are presented, which emit electron beams spinpolarized to a degree of P = 75% typically. Quantum yields around QE = 0.4% are observed routinely. The figure of merit P2 × QE = 2.3 × 10−3 is comparable to that of the best strained layer cathodes reported in literature. The optimum wavelength of irradiating light around 830 nm is in convenient reach of Ti:sapphire lasers or diode lasers respectively. The cathodes are produced using MOCVD-techniques. A GaAs.55P.45-GaAs.85P.15 superlattice structure prevents the migration of dislocations from the substrate and bottom layers to the strained overlayer. The surface is protected by an arsenic layer so that n…

Materials sciencebusiness.industrySuperlatticeGeneral ChemistrySubstrate (electronics)PhotocathodeCathodeOverlayerlaw.inventionOpticslawSapphireOptoelectronicsGeneral Materials ScienceQuantum efficiencybusinessMicrotronApplied Physics A Materials Science & Processing
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Transition radiation in the x-ray region from a low emittance 855 MeV electron beam

1997

A quasi-monochromatic hard x-ray beam with a photon energy of 33 keV has been produced from transition radiation (TR) at the Mainz Microtron MAMI. The radiator was a stack of 30 polyimide foils of 25 μm thickness and 75 μm separation and the monochromator a highly-oriented pyrolytic graphite crystal. The intrinsic bandwidth was measured with a critical absorption technique to be 100 eV. On the basis of these experiments a photon flux of 4⋅109/mm2s over an illuminated area of 5.7×125 mm2 can be expected from an optimized beryllium radiator at a beam current of 100 μA. At the K-absorption edge of titanium at 5 keV narrow band transition radiation has been observed from a stack of four foils o…

Materials sciencebusiness.industryX-rayPhoton energylaw.inventionOpticsTransition radiationlawCathode rayAtomic physicsbusinessAbsorption (electromagnetic radiation)MicrotronBeam (structure)MonochromatorThe 17th international conference on x-ray and inner-shell processes
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A short-orbit spectrometer for low-energy pion detection in electroproduction experiments at MAMI

2017

A new Short-Orbit Spectrometer (SOS) has been constructed and installed within the experimental facility of the A1 collaboration at Mainz Microtron (MAMI), with the goal to detect low-energy pions. It is equipped with a Browne-Buechner magnet and a detector system consisting of two helium-ethane based drift chambers and a scintillator telescope made of five layers. The detector system allows detection of pions in the momentum range of 50 - 147 MeV/c, which corresponds to 8.7 - 63 MeV kinetic energy. The spectrometer can be placed at a distance range of 54 - 66 cm from the target center. Two collimators are available for the measurements, one having 1.8 msr aperture and the other having 7 ms…

Nuclear and High Energy PhysicsPhysics - Instrumentation and DetectorsAperturePhysics::Instrumentation and DetectorsFOS: Physical sciencesScintillatorKinetic energy01 natural scienceslaw.inventionNuclear physicsTelescopePionlaw0103 physical sciencesNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentInstrumentationMicrotronPhysicslow-energy pion detectionSpectrometer010308 nuclear & particles physicsDetectorInstrumentation and Detectors (physics.ins-det)3. Good healthPhysics::Accelerator Physics
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Silicon Detector Telescope for proton detection in electron scattering reactions at MAMI

2012

Abstract A new Silicon Detector Telescope has been constructed and installed within the experimental facility of the A1 collaboration at Mainz Microtron, with the goal to detect low-energy protons. It consists of seven silicon layers for energy and angle measurement and a plastic scintillator for triggering purposes. The detector subtends a solid angle up to 88 msr, depending on the distance from the target and covers the proton kinetic energy range of 25–41  MeV with the mean energy resolution σ E = 0.47 MeV , operating at 500 kHz. Digital signal processing methods applied for energy reconstruction have been important for keeping the acceptable energy resolution at high counting rates. The…

Nuclear and High Energy PhysicsSiliconPhysics::Instrumentation and Detectorschemistry.chemical_elementScintillator01 natural scienceslaw.inventionNuclear physicsTelescopeOpticslaw0103 physical sciencessilicon detector; digital signal processing; electron scatteringNuclear Experiment010306 general physicsInstrumentationMicrotronPhysicsRange (particle radiation)Spectrometer010308 nuclear & particles physicsbusiness.industryDetectorSolid anglechemistryPhysics::Accelerator PhysicsbusinessNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Measurement of GEp/GMp via polarization transfer at Q2 = 0.4 GeV /c2

2001

The polarization transfer from longitudinally polarized electrons to protons in the elastic scattering p( e, e' p) has been measured around Q2 = 0.4 (GeV/c)2 with the three-spectrometer facility at the Mainz microtron MAMI. From this polarization transfer the ratio G Ep/(G Mp/μp) has been determined. The ratio is found to be slightly less than unity in agreement with recent results from other laboratories and from the Rosenbluth separation of cross-sections measured with unpolarized electrons.

Nuclear physicsElastic scatteringPhysicsNuclear and High Energy PhysicsHadronNuclear fusionElectronAtomic physicsPolarization (waves)MicrotronThe European Physical Journal A
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The search for dark matter gauge bosons with the Mainz Microtron

2011

Abstract A pilot experiment in the search for light gauge bosons at the spectrometer setup of the A1 collaboration at MAMI is presented. Light gauge bosons arise naturally in a wide range of theoretical approaches beyond the standard model and are in accordance with several pieces of experimental evidence not yet understood in the standard model. A first test measurement at MAMI showed that existing limits on the coupling of such a light gauge boson can be improved by nearly an order of magnitude by fixed target experiments at existing electron accelerators.

Nuclear physicsHidden sectorPhysicsNuclear and High Energy PhysicsGauge bosonParticle physicsSpectrometerPhysics beyond the Standard ModelHigh Energy Physics::PhenomenologyDark matterTechnicolorMicrotronStandard ModelProgress in Particle and Nuclear Physics
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