Search results for "Microtron"

showing 10 items of 149 documents

The three-spectrometer facility at the Mainz microtron MAMI

1998

Abstract A set-up of three high-resolution magnetic spectrometers, for simplicity named A, B and C, has been built as the central facility for the precise determination of double and triple coincidence cross sections of hadron knock-out and meson production through the scattering of electrons at the Mainz microtron MAMI. The spectrometers A and C with point-to-point optics in the dispersive plane and parallel-to-point optics in the non-dispersive plane have a solid angle of 28 msr and a momentum acceptance of 20 and 25%, respectively. They each consist of a quadrupole, a sextupole and two dipole magnets, reaching maximum momenta of 735 and 550 MeV/c, respectively. The spectrometer B has a s…

PhysicsNuclear and High Energy PhysicsSpectrometerCherenkov detectorSolid angleElectronlaw.inventionNuclear physicsDipoleDipole magnetlawQuadrupoleNuclear ExperimentInstrumentationMicrotronNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Efficiency studies for a tracking detector based on square 1.5m long scintillating fibers read out by SiPM

2009

Abstract A tracking detector based on 1.5 m long scintillating fibers is being developed for the electron arm of the KAOS spectrometer at the Mainz Microtron MAMI. Measurements on light attenuation, particle detection efficiencies and accidental coincidence rates with a prototype set-up using 2 × 2 mm 2 fibers read out by silicon photomultipliers (SiPM) are presented. The highest efficiency at the lowest accidental coincidence rate was reached for high trigger thresholds at the largest SiPM bias voltages. The influence of signal attenuation and dispersion on detection efficiencies is discussed. The results are in good agreement with a Monte Carlo model that was used to predict detector char…

PhysicsNuclear and High Energy PhysicsSpectrometerPhysics::Instrumentation and Detectorsbusiness.industryAttenuationMonte Carlo methodDetectorTracking (particle physics)Silicon photomultiplierOpticsDispersion (optics)OptoelectronicsNuclear ExperimentbusinessInstrumentationMicrotronNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Operation of the MAMI accelerator with a Wien filter based spin rotation system

2006

A compact spin rotation system based on a Wien filter has been installed at the Mainz microtron accelerator (MAMI). Under operation with varying spin rotation angles a significant change of focal length together with a shift of the central beam trajectory is expected. We demonstrate that these effects can be kept under control. As a consequence operation with spin rotation angles between 0° and ±90° has been achieved without compromising the beam quality and operational stability of MAMI.

PhysicsNuclear and High Energy PhysicsWien filterRotationNuclear physicsRotation systemBeam trajectoryPhysics::Accelerator PhysicsFocal lengthLaser beam qualityNuclear ExperimentSpin (physics)InstrumentationMicrotronNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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The first Virtual Compton Scattering experiment at MAMI

1999

Abstract Virtual Compton scattering, i.e. the exclusive reaction γ ∗ p → γ′p′ with γ ∗ denoting a virtual photon, provides new insights on the internal structure of the proton. Below π 0 production threshold, this experiment measures the generalized polarizabilities of the proton as defined by Guichon et al [1], [2] and Drechsel et al [3]. These new electromagnetic observables, functions of Q 2 , enlarge the concept of electric (α0 and magnetic (β) polarizabilities in Real Compton Scattering ( Q 2 =0) [4]. The first VCS experiment [5] of this kind was measured at the three spectrometer facility at the Mainz Microtron MAMI for Q 2 =0.33 GeV 2 and we present in this paper the preliminary resu…

PhysicsNuclear and High Energy Physics[PHYS.HEXP] Physics [physics]/High Energy Physics - Experiment [hep-ex]ProtonSpectrometer010308 nuclear & particles physicsCompton scatteringVirtual particleObservable01 natural sciences7. Clean energyNuclear physics0103 physical sciences[PHYS.HEXP]Physics [physics]/High Energy Physics - Experiment [hep-ex]Nuclear Experiment010306 general physicsMicrotron
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Novel digital K-edge imaging system with transition radiation from an 855-MeV electron beam

2001

A novel K-edge imaging method has been developed at the Mainz Microtron MAMI aiming at a very efficient use of the transition radiation (TR) flux generated by the external 855-MeV electron beam in a foil stack. A fan-like quasi-monochromatic hard X-ray beam is produced from the /spl plusmn/1-mrad-wide TR cone with a highly oriented pyrolytic graphite (HOPG) crystal. The absorption of the object in front of a 30 mm/spl times/10 mm pn charge-coupled device (pn-CCD) photon detector is measured at every pixel by a broad-band energy scan around the K-absorption edge. This is accomplished by a synchronous variation of the lateral crystal position and the electron beam direction which defines also…

PhysicsNuclear and High Energy Physicsbusiness.industryDetectorchemistry.chemical_elementImaging phantomXenonOpticsNuclear Energy and EngineeringTransition radiationK-edgechemistryHighly oriented pyrolytic graphiteCathode rayElectrical and Electronic EngineeringbusinessMicrotronIEEE Transactions on Nuclear Science
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A Compact Solid State Detector for Small Angle Particle Tracking

1999

MIDAS (MIcrostrip Detector Array System) is a compact silicon tracking telescope for charged particles emitted at small angles in intermediate energy photonuclear reactions. It was realized to increase the angular acceptance of the DAPHNE detector and used in an experimental program to check the Gerasimov-Drell-Hearn sum rule at the Mainz electron microtron, MAMI. MIDAS provides a trigger for charged hadrons, p/pi identification and particle tracking in the region 7 deg < theta < 16 deg. In this paper we present the main characteristics of MIDAS and its measured performances.

PhysicsNuclear and High Energy Physicsbusiness.industryPhysics::Instrumentation and DetectorsDetectorHadronNuclear TheoryFOS: Physical sciencesElectronTracking (particle physics)nucl-exCharged particlelaw.inventionTelescopeOpticslawHigh Energy Physics::ExperimentSum rule in quantum mechanicsNuclear Experiment (nucl-ex)businessNuclear ExperimentInstrumentationMicrotronNuclear Experiment
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A highly polarized target for the electron beam at MAMI

2009

Abstract Polarized He 3 from metastability exchange optical pumping (MEOP) is used as an effective polarized neutron target for electron scattering experiments at the MAinz MIcrotron (MAMI). With the present setup an initial polarization of up to 72% has been obtained at the experimental area. A novel calibration technique will be presented which allows the determination of the absolute polarization within a relative uncertainty of 3%.

PhysicsNuclear and High Energy Physicsbusiness.industryPolarization (waves)Polarized targetOptical pumpingNuclear physicsOpticsMetastabilityCathode rayNeutronNuclear ExperimentbusinessInstrumentationMicrotronElectron scatteringNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Double- π0 photoproduction from the deuteron

2000

The photoproduction of two neutral pions from the deuteron has been studied for incident photon energies from 200 MeV to 820 MeV with the TAPS spectrometer at MAMI (Mainz Microtron). The total cross-section was determined and used to deduce the cross-section from the neutron. Due to the good statistical quality of the data Dalitz plots for the three particles in the exit channel (pi (0)pi N-0) could be constructed. The invariant mass distributions derived from them are presented in this paper. They indicate that the important reaction mechanism in the second resonance region is a sequential decay pattern involving the population of the Delta (1232)-resonance as an intermediate state.

PhysicsNuclear and High Energy Physicseducation.field_of_study010308 nuclear & particles physicsNuclear TheoryHadronPopulation01 natural sciencesResonance (particle physics)Nuclear physicsPionDeuterium0103 physical sciencesNeutronInvariant massAtomic physicsNuclear Experiment010306 general physicseducationMicrotronThe European Physical Journal A
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Beam parameter stabilization for the P2 experiment at MESA

2020

Abstract The P2 Experiment at MESA (Mainz Energy-recovering Superconducting Accelerator) will measure the weak mixing angle via electron proton scattering at 155 MeV. The expected measured parity violation asymmetry will be about 40 ppb. This requires a high precision beam diagnostic and control system in order to minimize asymmetries that derive from helicity correlated fluctuations of the beam parameters. A control system for position and angle has been installed and tested at MAMI (Mainz Microtron) and the P2 precision requirements for determining the asymmetry and controlling the transverse beam parameters have been met.

PhysicsNuclear and High Energy Physicsmedia_common.quotation_subjectParity (physics)ElectronHelicityAsymmetryMesaNuclear physicsControl systemProton scatteringPhysics::Accelerator PhysicsNuclear ExperimentInstrumentationcomputerMicrotroncomputer.programming_languagemedia_commonNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Spinrotator for MAMI

1991

A source of polarized electrons based on the photoemission of a GaAsP-cathode [1] has been set up to inject polarized electrons in the Mainz microtron MAMI. In order to compensate the spin precession in MAMI a spinrotator system has to be integrated in the 100 keV beamline from the source to the injector linac to achieve the required longitudinal spin direction at target position.

PhysicsNuclear physicsBeamlinePhysics::Instrumentation and DetectorsPrecessionPhysics::Accelerator PhysicsCondensed Matter::Strongly Correlated ElectronsElectronNuclear ExperimentSpin (physics)Precession angleMicrotronLinear particle accelerator
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