Search results for "Microtron"

showing 10 items of 149 documents

Experimental study of theγp→ηpreaction with the Crystal Ball detector at the Mainz Microtron (MAMI-C)

2010

The gamma p - = W >= 1.87 GeV). Bremsstrahlung photons produced by the 1.5-GeV electron beam of the Mainz Microtron MAMI-C and momentum analyzed by the Glasgow tagging spectrometer were used for the eta-meson production. Our accumulation of 3.8 x 10(6) gamma p -< eta p -< 3 pi(0) p -< 6 gamma p events allows a detailed study of the reaction dynamics. The gamma p -< eta p differential cross sections were determined for 120 energy bins and the full range of the production angles. Our data show a dip near W = 1680 MeV in the total cross section caused by a substantial dip in eta production at forward angles. The data are compared to predictions of previous SAID and MAID partial-wave analyses a…

PhysicsNuclear and High Energy PhysicsMeson010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaPartial wave analysisHadronBremsstrahlung01 natural sciencesNuclear physicsParticle decay0103 physical sciencesNuclear Experiment010306 general physicsNucleonMicrotronCrystal BallPhysical Review C
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C(,pn) photon asymmetry for Eγ=180–340 MeV

1999

The photon asymmetry (Σ) of the 12C(,pn) reaction has been measured using linearly polarised tagged photons at the Mainz microtron MAMI for Eγ=180–340 MeV. The data have been analysed in separate missing energy (Em) regions corresponding to the ejection of nucleons from (1p)2 and (1p)(1s) shells. The measured Σ values for both Em regions are smaller in magnitude than corresponding 2H data, but the (1p)2 results have a similar Eγ dependence. Calculations of direct two-nucleon emission overestimate the magnitude of Σ at all photon energies.

PhysicsNuclear and High Energy PhysicsMissing energyPhotonmedia_common.quotation_subjectNuclear TheoryAsymmetryNuclear physicsMagnitude (astronomy)Atomic physicsNuclear ExperimentNucleonMicrotronmedia_commonPhysics Letters B
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Determination of the neutron electric form factor in the D(e,e′n)p reaction and the influence of nuclear binding

1999

The electric form factor of the neutron GE,n has been determined at the Mainz Microtron MAMI at the low momentum transfer Q2= 0.15 (GeV/c)2 in a measurement of the recoil polarisation ratio Px/Pz in the quasifree reaction D(e,e′n)p. At this Q2 the influence of the nuclear binding is strong. A purely kinematical model is used to get some insight into the effect of the initial Fermi momentum distribution of the neutron. The influence of the final state interaction is determined quantitatively by a model of Arenhovel et al.. After the corresponding corrections a value of GE,n(0.15 (GeV/c)2) = 0.0481±0.0065stat±0.0053syst is obtained.

PhysicsNuclear and High Energy PhysicsNuclear TheoryMomentum transferHadronElectric form factor(n-p) reactionNuclear physicsRecoilNuclear fusionNeutronAtomic physicsNuclear ExperimentMicrotronThe European Physical Journal A
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New determination of theηtransition form factor in the Dalitz decayη→e+e−γwith the Crystal Ball/TAPS detectors at the Mainz Microtron

2014

The Dalitz decay eta -> e(+) e(-) gamma has been measured in the gamma p -> eta p reaction with the Crystal Ball and TAPS multiphoton spectrometers, together with the photon-tagging facility at the Mainz Microtron MAMI. The experimental statistic used in this work is one order of magnitude greater than in any previous measurement of eta -> e(+) e(-) gamma. The value obtained for the slope parameter Lambda(-2) of the eta transition form factor, Lambda(-2) = (1.95 +/- 0.15(stat) +/- 0.10(syst)) GeV-2, is in good agreement with recent measurements conducted in eta -> e(+) e(-) gamma and eta -> mu(+) mu(-) gamma decays, as well as with recent form-factor calculations. The uncertainty obtained i…

PhysicsNuclear and High Energy PhysicsParticle physics010308 nuclear & particles physicsDetectorForm factor (quantum field theory)Gamma rayLambda01 natural sciencesNuclear physics0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment010306 general physicsMicrotronCrystal BallPhysical Review C
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THE BARYON RESONANCE PROGRAM AT MAMI

2010

The Mainz Microtron MAMI is an ideal facility to study the hadron structure with the electromagnetic probe. With the fourth accelerator stage (MAMI-C) which went into operation in 2007 high-intensity polarized electron and photon beams with energies up to 1.5 GeV are delivered to the experiments. Polarized targets and recoil polarimeters in combination with dedicated detectors are available for precision experiments in hadron physics. In this article, an overview over selected recent results on the study of low-lying baryon resonances and future perspectives will be given.

PhysicsNuclear and High Energy PhysicsParticle physicsHadronGeneral Physics and AstronomyResonanceElectronNuclear physicsBaryonRecoilHadron physicsPhoton beamsNuclear ExperimentMicrotronInternational Journal of Modern Physics E
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Pion electroproduction in the 3He(e,é π+)3H reaction at intermediate energies

1997

Abstract The differential coincident pion electroproduction cross section in the 3 He(e,e π + ) 3 H reaction has been measured with high resolution with the three-spectrometer set-up at the Mainz Microtron (MAMI) electron accelerator. Measurements were performed at the four incident energies E 0 = 855, 675, 600, and 555 MeV at fixed four-momentum transfer Q 2 = 0.045 GeV 2 , with the pions detected in parallel kinematics. This enables a separation of the measured cross section into the transverse and longitudinal structure functions by means of the Rosenbluth method. The experimental data are compared to model calculations, in which the elementary pion production amplitude includes the stan…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryParticle acceleratorResonance (particle physics)law.inventionNuclear physicsCross section (physics)AmplitudePionCoincidentlawHigh Energy Physics::ExperimentNuclear ExperimentWave functionMicrotronNuclear Physics A
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Near threshold photoproduction of η mesons from 4 He

1999

Photoproduction of η mesons from 4He has been measured for the first time. The experiment was performed at the Mainz Microtron (MAMI) using the TAPS photon spectrometer and the Glasgow/Mainz tagged photon facility. η mesons were identified in coincidence with recoil nucleons. Total and differential cross sections are presented in the photon energy range between threshold and 818 MeV. The exclusive data are used to determine the ratio of the elementary production cross sections on bound neutrons and protons, σn/σp= 0.68 ± 0.02 ± 0.09. In addition, upper limits for the total coherent cross section have been derived.

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonMeson010308 nuclear & particles physicsNuclear TheoryHadronPhoton energy01 natural sciences7. Clean energyNuclear physicsRecoil0103 physical sciencesHigh Energy Physics::ExperimentNeutronNuclear Experiment010306 general physicsNucleonMicrotronThe European Physical Journal A
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Overview of the electromagnetic production of strange mesons at MAMI

2013

Abstract The Mainz Microtron MAMI provides a continuous-wave unpolarized or spin-polarized electron beam with energies up to 1.6 GeV and high degrees of polarization. Electro-production of strange mesons is performed in the multi-spectrometer facility with the Kaos spectrometer for kaon detection and a high-resolution spectrometer for electron detection in plane or out of plane. Differential cross section measurements of exclusive p ( e , e ′ K + ) Λ , Σ 0 reactions at low four-momentum transfers in the nucleonʼs third resonance region have been done, followed by a measurement of the beam helicity asymmetry for p ( e → , e ′ K + ) Λ . These studies are important for the understanding of the…

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonMesonHadronStrangenessLambda baryonHelicitySigma baryonNuclear physicsstrangeness reactions; kaon electro-production; missing mass spectroscopy; structure functionsNuclear ExperimentMicrotronNuclear Physics A
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Photoproduction of theωmeson on the proton near threshold

2015

An experimental study of omega photoproduction on the proton was conducted by using the Crystal Ball and TAPS multiphoton spectrometers together with the photon tagging facility at the Mainz Microtron MAMI. The gamma p -> omega p differential cross sections are measured from threshold to the incident-photon energy E-gamma = 1.40 GeV (W = 1.87 GeV for the center-of-mass energy) with 15-MeV binning in E-gamma and full production-angle coverage. The quality of the present data near threshold gives access to a variety of interesting physics aspects. As an example, an estimation of the omega N scattering length alpha(omega p) is provided.

PhysicsNuclear and High Energy PhysicsParticle physicsPhotonProtonMesonVector meson dominanceScattering length7. Clean energyOmegaNuclear physicsNuclear ExperimentMicrotronCrystal BallPhysical Review C
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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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