0000000000003763

AUTHOR

J. C. Mcgeorge

showing 68 related works from this author

(γ,2N) reaction inC12

1995

The $^{12}$C(\ensuremath{\gamma},pn) and $^{12}$C(\ensuremath{\gamma},pp) reactions have been measured for photon energies between 80 and 157 MeV using a photon tagging spectrometer and plastic scintillator detectors. The overall energy resolution was \ensuremath{\sim}7 MeV, sufficient to determine the initial shells of the emitted nucleons. Corrections were made for solid angle and threshold effects by means of Monte Carlo simulations. For the (\ensuremath{\gamma},pn) reaction both the missing energy and recoil momentum distributions are largely consistent with a two-nucleon absorption process on p-shell an sp nucleon pairs. For the much smaller $^{12}$C(\ensuremath{\gamma},pp) cross secti…

PhysicsMomentumNuclear and High Energy PhysicsPhotonMissing energyRecoilNuclear TheoryAbsorption (logic)Atomic physicsScintillatorNuclear ExperimentNucleonEnergy (signal processing)Physical Review C
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Test of Low-Energy Theorems forH1(γ→,π0)H1in the Threshold Region

2001

The photon asymmetry in the reaction H-1(, pi (0))H-1 close to threshold has been measured for the first time with the photon spectrometer TAPS using linearly polarized photons from the tagged-photon facility at the Mainz Microtron MAMI. The total and differential cross sections were also measured simultaneously with the photon asymmetry. This allowed determination of the S-wave and all three P-wave amplitudes. The values obtained at threshold are E0+ = [-1.33 +/- 0.08(stat) +/- 0.03(syst)] x 10(-3)/m(pi+), P-1 = [9.47 +/- 0.08(stat) +/- 0.29(syst)] x 10(-3)q /m(pi+)(2) P-2 [-9.46 +/- 0.1(stat) +/- 0.29(syst)] x 10(-3)q/m(pi+)(2), and P-3 = [11.48 +/- 0.06(stat) +/- 0.35(syst)] x 10(-3)q/m(…

PhysicsPhotonLow energy010308 nuclear & particles physics0103 physical sciencesPiAnalytical chemistryGeneral Physics and Astronomy010306 general physics01 natural sciencesNuclear theoryMicrotronPhysical Review Letters
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Double pi(0) photoproduction off the proton at threshold

2003

The reaction $\gamma p \to \pi^0 \pi^0 p$ has been measured using the TAPS BaF$_2$ calorimeter at the tagged photon facility of the Mainz Microtron accelerator. Chiral perturbation theory (ChPT) predicts that close to threshold this channel is significantly enhanced compared to double pion final states with charged pions. In contrast to other reaction channels, the lower order tree terms are strongly suppressed in 2$\pi^0$ photoproduction. The consequence is the dominance of pion loops in the 2$\pi^0$ channel close to threshold - a result that opens new prospects for the test of ChPT and in particular its inherent loop terms. The present measurement is the first which is sensitive enough fo…

PhysicsTAPSNuclear and High Energy PhysicsParticle physicsChiral perturbation theoryMesonProtonNuclear TheoryHigh Energy Physics::LatticeNEUTRAL-PION-PHOTOPRODUCTIONHadronNuclear TheoryElementary particleCHIRAL PERTURBATION-THEORYNuclear physicsPionTAGGED PHOTON SPECTROMETERNucleonNuclear ExperimentMicrotronNuclear Experiment
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Determination of theE2/M1ratio in theγN→Δ(1232)transition from a simultaneous measurement ofp(γ→,p)π0andp(γ→,π+)n

2000

Tagged linearly polarized photons have been used at the Mainz Microtron (MAMI) for simultaneous measurements of the $p(\stackrel{\ensuremath{\rightarrow}}{\ensuremath{\gamma}},p){\ensuremath{\pi}}^{0}$ and $p(\stackrel{\ensuremath{\rightarrow}}{\ensuremath{\gamma}},{\ensuremath{\pi}}^{+})n$ reaction channels to study the $\ensuremath{\gamma}\stackrel{\ensuremath{\rightarrow}}{N}\ensuremath{\Delta}(1232)$ transition. The energy dependence of the magnetic dipole ${M}_{1+}^{3/2}$ and electric quadrupole ${E}_{1+}^{3/2}$ amplitudes have been extracted from these data in the photon energy range from $270$ to 420 MeV. The $E2/M1$ ratio for the $\ensuremath{\gamma}\stackrel{\ensuremath{\rightarrow…

PhysicsNuclear and High Energy PhysicsParticle physicsMeson productionHigh Energy Physics::PhenomenologyResonancePhoton energyAngular distributionQuadrupolePiAtomic physicsNuclear ExperimentNuclear theoryEnergy (signal processing)Physical Review C
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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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Double pion photoproduction off nuclei - Are there effects beyond final-state interaction?

2013

Photoproduction of $\pi^{0}\pi^{0}$ and $\pi^{0}\pi^{\pm}$ pairs from nuclei has been measured over a wide mass range ($^2$H, $^{7}$Li, $^{12}$C, $^{40}$Ca, and $^{\rm nat}$Pb) for photon energies from threshold to 600 MeV. The experiments were performed at the MAMI accelerator in Mainz, using the Glasgow photon tagging spectrometer and a 4$\pi$ electromagnetic calorimeter consisting of the Crystal Ball and TAPS detectors. A shift of the pion-pion invariant mass spectra for heavy nuclei to small invariant masses has been observed for $\pi^0$ pairs but also for the mixed-charge pairs. The precise results allow for the first time a model-independent analysis of the influence of pion final-sta…

PhysicsNuclear and High Energy PhysicsParticle physicsdouble pion photoproduction; crystal ball; sigma-in-medium modificationPhotonMeson010308 nuclear & particles physicsHadronNuclear TheoryCarbon-12FOS: Physical sciencesElementary particle01 natural sciences7. Clean energyNuclear physicsMassless particlePion0103 physical sciencesHigh Energy Physics::ExperimentNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentCrystal Ball
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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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Dependence of the C12(γ→,pd) reaction on photon linear polarisation

2007

Abstract The sensitivity of the C 12 ( γ → , pd ) reaction to photon linear polarisation has been determined at MAMI, giving the first measurement of the reaction for a nucleus heavier than 3He. Photon asymmetries and cross sections were measured for E γ = 170 to 350 MeV. For E γ below the Δ resonance, reactions leaving the residual 9Be near its ground state show a positive asymmetry of up to 0.3, similar to that observed for 3He suggesting a similar reaction mechanism for the two nuclei.

PhysicsNuclear and High Energy PhysicsReaction mechanismPhotonmedicine.anatomical_structuremedia_common.quotation_subjectmedicineResonanceAtomic physicsGround stateAsymmetryNucleusmedia_commonPhysics Letters B
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Quasifreeπ+production studied using theC12(γ, π+n)B11reaction in theΔ(1232)resonance region

1996

Results are presented from a coincidence study of the {sup 12}C({gamma},{pi}{sup +}{ital n}){sup 11}B quasifree pion production reaction made in the {Delta}-resonance region using tagged photons. Cross sections for reactions originating on 1{ital p}-shell protons are found to be significantly larger than predicted by calculations based on quasifree pion production. It is suggested that more sophisticated calculations, perhaps including medium effects, may be required to reproduce the data. {copyright} {ital 1996 The American Physical Society.}

PhysicsNuclear and High Energy PhysicsPhotonPionMeson productionPiProduction (computer science)Atomic physicsResonance (particle physics)Physical Review C
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Photon Asymmetry of Deuteron Photodisintegration Between 160 and 410 MeV

1999

The photon asymmetry Σ of the reaction has been measured across the photon energy range 160–410 MeV at the Mainz Microtron MAMI. Linearly polarized photons were obtained from coherent bremsstrahlung and their energies were determined with the Glasgow tagging spectrometer. The large acceptance detector DAPHNE enabled the outgoing protons to be measured over the complete azimuthal range and for polar angles from 35° to 155° in the c.m. system. The data are compared with existing results and recent theoretical calculations.

PhysicsRange (particle radiation)PhotonSpectrometermedia_common.quotation_subjectBremsstrahlungPhoton energyAsymmetryAtomic and Molecular Physics and OpticsNuclear physicsPhotodisintegrationPhysics::Accelerator PhysicsAtomic physicsNuclear ExperimentMicrotronmedia_commonFew-Body Systems
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New results on the Roper resonance and the P_{11} partial wave

2008

Properties of the Roper resonance, the first scalar excitation of the nucleon, are determined. Pole positions and residues of the $P_{11}$ partial wave are studied in a combined analysis of pion- and photo-induced reactions. We find the Roper pole at $\{(1371\pm7)-i(92\pm10)\}$ MeV and an elasticity of $0.61\pm 0.03$. The largest decay coupling is found for the $N\sigma$ ($\sigma=(\pi\pi)$-$S$-wave). The analysis is based on new data on $\gamma p\to p\pi^0\pi^0$ for photons in the energy range from the two-pion threshold to 820 MeV from TAPS at Mainz and from 0.4 to 1.3 GeV from Crystal Barrel at Bonn and includes further data from other experiments. The partial wave analysis excludes the p…

TAPSNuclear and High Energy PhysicsRoper resonancePhotonProtonPHOTON SPECTROMETERPartial wave analysisNuclear TheoryDalitz plotFOS: Physical sciencesPION-PHOTOPRODUCTIONPROTONTHRESHOLDNuclear physicsPionHigh Energy Physics - Phenomenology (hep-ph)Nuclear ExperimentPhysicsPI(0) PHOTOPRODUCTIONHigh Energy Physics - PhenomenologyRELATIVISTIC QUARK-MODELSTRANGE-BARYON SPECTRUMPOSITIVE-STRANGENESSFORCESNucleonExcitation
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Coherent photoproduction of η-mesons off 3He – search for η-mesic nuclei

2012

Coherent photoproduction of $\eta$-mesons off $^3$He, i.e. the reaction $\gamma ^3{He}\rightarrow \eta ^3{He}$, has been investigated in the near-threshold region. The experiment was performed at the Glasgow tagged photon facility of the Mainz MAMI accelerator with the combined Crystal Ball - TAPS detector. Angular distributions and the total cross section were measured using the $\eta\rightarrow \gamma\gamma$ and $\eta\rightarrow 3\pi^0\rightarrow 6\gamma$ decay channels. The observed extremely sharp rise of the cross section at threshold and the behavior of the angular distributions are evidence for a strong $\eta {^3{He}}$ final state interaction, pointing to the existence of a resonant …

PhysicsExcitation functionNuclear and High Energy PhysicsParticle physicsMesonHigh Energy Physics::PhenomenologyHadronGamma rayFOS: Physical sciencesBaryonNuclear physicsHigh Energy Physics::ExperimentNuclear Experiment (nucl-ex)total cross section ; photoproduction ; eta meson ; final-state interaction ; Crystal Ball ; MAMINucleonNuclear ExperimentNuclear ExperimentIsotopes of heliumCrystal Ball
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Photoproduction of $\eta$ $\pi$ pairs off nucleons and deuterons

2016

Quasi-free photoproduction of $\pi\eta$-pairs has been investigated from threshold up to incident photon energies of 1.4 GeV, respectively up to photon-nucleon invariant masses up to 1.9 GeV. Total cross sections, angular distributions, invariant-mass distributions of the $\pi\eta$ and meson-nucleon pairs, and beam-helicity asymmetries have been measured for the reactions $\gamma p\rightarrow p\pi^0\eta$, $\gamma n\rightarrow n\pi^0\eta$, $\gamma p\rightarrow n\pi^+\eta$, and $\gamma n\rightarrow p\pi^-\eta$ from nucleons bound inside the deuteron. For the $\gamma p$ initial state data for free protons have also been analyzed. Finally, the total cross sections for quasi-free production of $…

PhysicsNuclear and High Energy PhysicsPhotonProton010308 nuclear & particles physicsNuclear TheoryFOS: Physical sciences01 natural sciences7. Clean energyNuclear physicsDeuteriumREACTION GAMMA-P ; TAGGED PHOTON SPECTROMETER ; I-CIRCLE-DOT ; MESON PHOTOPRODUCTION ; HIGH-STATISTICS ; PROTON ; THRESHOLD ; MAMI ; POLARIZATION ; PI(0)-PAIRS0103 physical sciencesPiNeutronHigh Energy Physics::Experimentddc:530Decay chainNuclear Experiment (nucl-ex)010306 general physicsNucleonNuclear ExperimentNuclear ExperimentCrystal Ball
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Investigation of multiparticle final states in12C photoreactions

1998

The ${}^{12}\mathrm{C}(\ensuremath{\gamma},pn)$, ${}^{12}\mathrm{C}(\ensuremath{\gamma},pp)$, ${}^{12}\mathrm{C}(\ensuremath{\gamma},ppp)$, ${}^{12}\mathrm{C}(\ensuremath{\gamma},pp{\ensuremath{\pi}}^{\ifmmode\pm\else\textpm\fi{}})$, ${}^{12}\mathrm{C}(\ensuremath{\gamma},p{\ensuremath{\pi}}^{\ifmmode\pm\else\textpm\fi{}})$ reactions have been studied using tagged photons of energy ${E}_{\ensuremath{\gamma}}=250$--600 MeV. A model which includes all major absorption mechanisms and final state interactions gives results that agree well with the shapes of missing energy spectra, but for some channels the predicted cross sections are too large.

PhysicsNuclear and High Energy PhysicsPionAstrophysics::High Energy Astrophysical PhenomenaAbsorption (logic)Atomic physicsSpectral lineEnergy (signal processing)Physical Review C
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The isospin structure of photoproduction of πη pairs from the nucleon in the threshold region

2015

Abstract Photoproduction of πη-pairs from nucleons has been investigated from threshold up to incident photon energies of ≈ 1.4 GeV. The quasi-free reactions γ p → p π 0 η , γ n → n π 0 η , γ p → n π + η , and γ n → p π − η were for the first time measured from nucleons bound in the deuteron. The corresponding reactions from a free-proton target were also studied to investigate final-state interaction effects (for neutral pions the free-proton results could be compared to previous measurements; the γ p → n π + η reaction was measured for the first time). For the π 0 η final state coherent production via the γ d → d π 0 η reaction was also investigated. The experiments were performed at the …

PhysicsNuclear and High Energy PhysicsPhotonPhysicsNuclear Theory7. Clean energylcsh:QC1-999photoproduction; final-state interaction; total cross section; Delta(1232) structure; deuteron; isospin; MAMIPionElectromagnetic calorimeterDeuteriumIsospinIsobarAtomic physicsNuclear ExperimentNucleonlcsh:PhysicsCrystal BallPhysics Letters B
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The 16O(γ, 2N) reaction measured with tagged photons

1991

The results of tagged-photon measurements of the 4He(γ, pn)d, 4He(γ, pn)pn and 4He(γ, pp)nn reactions, carried out with photons of energies 80–131 MeV, are presented. The (γ, pn)d three-body-breakup cross section dominates the four-body-breakup cross section. The three-body-breakup cross section and the corresponding deuteron recoil-momentum spectrum are reasonably accounted for by a mechanism of photon absorption on correlated proton-neutron pairs. In contrast the four-body-breakup mechanism appears to have two components: absorption on correlated proton-neutron pairs and a more complex additional component which has a distribution similar to phase space. The data rule out substantial phot…

Nuclear reactionPhysicsNuclear and High Energy PhysicsCross section (physics)Distribution (mathematics)PhotonDeuteriumPhase spaceNuclear TheoryAtomic physicsNuclear ExperimentAbsorption (electromagnetic radiation)Nuclear Physics A
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The reaction at Eγ = 60 and 80 MeV

1986

Abstract The tagged photon technique has been used to measure the 12C photoproton cross section over the angular range θp = 30°–135° for Eγ = 60 and 80 MeV. Comparison of the results with quasifree knockout and quasideuteron calculations shows that photon interaction with two-nucleon pairs is dominant at least for high excitation energies in the residual nucleus.

PhysicsNuclear and High Energy PhysicsAngular rangePhotonNuclear TheoryMeasure (physics)ResidualNuclear physicsCross section (physics)medicine.anatomical_structuremedicineAtomic physicsNuclear ExperimentNucleusExcitationPhysics Letters B
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Quasi-free Compton Scattering and the Polarizabilities of the Neutron

2002

Differential cross sections for quasi-free Compton scattering from the proton and neutron bound in the deuteron have been measured using the Glasgow/Mainz tagging spectrometer at the Mainz MAMI accelerator together with the Mainz 48 cm $\oslash$ $\times$ 64 cm NaI(Tl) photon detector and the G\"ottingen SENECA recoil detector. The data cover photon energies ranging from 200 MeV to 400 MeV at $\theta^{LAB}_\gamma=136.2^\circ$. Liquid deuterium and hydrogen targets allowed direct comparison of free and quasi-free scattering from the proton. The neutron detection efficiency of the SENECA detector was measured via the reaction $p(\gamma,\pi^+ n)$. The "free" proton Compton scattering cross sect…

Nuclear and High Energy PhysicsProtonNuclear TheoryFOS: Physical sciences7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentNuclear physicsHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Polarizability0103 physical sciencesNeutron detectionNeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysics010308 nuclear & particles physicsScatteringCompton scatteringHigh Energy Physics - PhenomenologyDeuteriumCover (topology)High Energy Physics::Experiment
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Measurement of the p(γ,π^{0}) cross section at threshold

1990

Differential and absolute cross sections for the reaction {ital p}({gamma},{pi}{sup 0}) have been measured with energy-defined photons in the threshold region ({ital E}{sub {gamma}}=131.4--157.2 MeV). The {ital E}{sub 0+} amplitude has been extracted out of the data. The values found are in disagreement with predictions of low-energy theorems.

Nuclear reactionPhysicsPhotonAmplitudePionMesonComputer Science::Information RetrievalHadronGeneral Physics and AstronomyElementary particleAtomic physicsBosonPhysical Review Letters
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Differential cross sections for coherent and incoherent neutral-pion photoproduction from calcium

1989

Differential and absolute cross sections for the coherent reaction $^{40}\mathrm{Ca}$(\ensuremath{\gamma},${\ensuremath{\pi}}^{0}$${)}^{40}$Ca g.s., as well as for the incoherent reaction $^{40}\mathrm{Ca}$(\ensuremath{\gamma},${\mathrm{\ensuremath{\pi}}}^{0}$${)}^{40}$Ca(g.s.), have been measured with monochromatic photons in the threshold region (${E}_{\ensuremath{\gamma}}$=157--169 MeV). The differential cross section for the coherent process exhibits a diffraction minimum due to the nuclear mass form factor while the incoherent cross section is rather structureless. The cross sections are in good agreement with recent distorted-wave impulse-approximation calculations.

PhysicsNuclear reactionPionMesonHadronForm factor (quantum field theory)General Physics and AstronomyElementary particleAtomic physicsDelta baryonBosonPhysical Review Letters
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Neutron Skin ofPb208from Coherent Pion Photoproduction

2014

Information on the size and shape of the neutron skin on (208)Pb is extracted from coherent pion photoproduction cross sections measured using the Crystal Ball detector together with the Glasgow tagger at the MAMI electron beam facility. On exploitation of an interpolated fit of a theoretical model to the measured cross sections, the half-height radius and diffuseness of the neutron distribution are found to be c(n)=6.70±0.03(stat.)  fm and a(n)=0.55±0.01(stat.)(-0.03)(+0.02)(sys.)  fm, respectively, corresponding to a neutron skin thickness Δr(np)=0.15±0.03(stat.)(-0.03)(+0.01)(sys.)  fm. The results give the first successful extraction of a neutron skin thickness with an electromagnetic p…

PhysicsEquation of stateMeson010308 nuclear & particles physicsScatteringGeneral Physics and AstronomyRadius01 natural sciencesNuclear physicsPion0103 physical sciencesHigh Energy Physics::ExperimentNeutronNuclear Experiment010306 general physicsMicrotronCrystal BallPhysical Review Letters
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In-Medium Properties of theD13(1520) Nucleon Resonance

2001

The in-medium properties of the ${\mathrm{D}}_{13}(1520)$ nucleon resonance were studied via photoproduction of ${\ensuremath{\pi}}^{0}$ mesons from nuclei (C, Ca, Nb, Pb) with the TAPS detector at the Mainz Microton accelerator. The inclusive (single and multiple pion production) data disagree with model predictions which explain the disappearance of the second resonance bump in total photoabsorption via a medium modification of the ${\mathrm{D}}_{13}\ensuremath{\rightarrow}\mathrm{N}\ensuremath{\rho}$ decay. The exclusive single ${\ensuremath{\pi}}^{0}$ production data show no broadening of the resonance structure beyond Fermi smearing. Both results together cast doubt on attempts to expl…

PhysicsParticle physicsPionMesonNuclear TheoryGeneral Physics and AstronomyProduction (computer science)Nuclear ExperimentNucleonResonance (chemistry)Fermi Gamma-ray Space TelescopePhysical Review Letters
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Search for the charge-conjugation-forbidden decayω→ηπ0

2009

A new upper limit of 2.3x10{sup -4} on the branching ratio of the decay {omega}{yields}{eta}{pi}{sup 0} has been obtained using the Crystal Ball multiphoton spectrometer at the Mainz Microtron MAMI. This decay is forbidden by charge-conjugation invariance of the strong and electromagnetic interactions. We have also obtained the upper limit of 2.3x10{sup -4} for the forbidden decay {omega}{yields}3{pi}{sup 0} and the upper limit of 2.4x10{sup -4} for {omega}{yields}2{pi}{sup 0}.

PhysicsNuclear and High Energy PhysicsParticle physicsParticle decayPionMesonBranching fractionHadronAtomic physicsNuclear ExperimentOmega baryonOmegaCrystal BallPhysical Review C
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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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Determination of the η-transition form factor in the γp→pη→pγe+e− reaction

2011

The Dalitz decay η→γe+e− has been measured using the combined Crystal Ball and TAPS photon detector setup at the electron accelerator MAMI-C. Compared to the most recent transition form-factor measurement in the e+e− channel, statistics have been improved by one order of magnitude. The e+e− invariant mass distribution shows a deviation from the QED prediction for a point-like particle, which can be described by a form-factor. Using the usual monopole transition form-factor parameterization, F(m2)=(1−m2/Λ2)−1, a value of Λ−2=(1.92±0.35(stat)±0.13(syst)) GeV−2 has been determined. This value is in good agreement with a recent measurement of the η Dalitz decay in the μ+μ− channel and with rece…

PhysicsNuclear and High Energy PhysicsMass distribution010308 nuclear & particles physicsPoint particleBranching fractionForm factor (quantum field theory)Particle accelerator01 natural scienceslaw.inventionNuclear physicslaw0103 physical sciencesHigh Energy Physics::ExperimentInvariant massNuclear Experiment010306 general physicsOrder of magnitudeCrystal BallPhysics Letters B
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Beam-Helicity Asymmetries in Double-Pion Photoproduction off the Proton

2009

Beam-helicity asymmetries have been measured at the MAMI accelerator in Mainz in the three isospin channels $\vec{\gamma}p\to \pi^{+}\pi^0n$, $\vec{\gamma}p\to \pi^{0}\pi^0p$ and $\vec{\gamma}p\to \pi^{+}\pi^{-}p$ . The circularly polarized photons, produced from bremsstrahlung of longitudinally polarized electrons, were tagged with the Glasgow magnetic spectrometer. Charged pions and the decay photons of $\pi^0$ mesons were detected in a $~4\pi$ electromagnetic calorimeter which combined the Crystal Ball detector with the TAPS detector. The precisely measured asymmetries are very sensitive to details of the production processes and are thus key observables in the modeling of the reaction d…

PhysicsParticle physicsProtonMeson010308 nuclear & particles physicsNuclear TheoryHadronFOS: Physical sciencesGeneral Physics and Astronomy7. Clean energy01 natural sciencesHelicity3. Good healthNuclear physicsPair productionPion0103 physical sciencesHigh Energy Physics::ExperimentInvariant massNuclear Experiment (nucl-ex)Nuclear Experiment010306 general physicsNuclear Experimentbeam-helicity asymmetries ; charged pions and the decay photonLeptonPhysical Review Letters
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Photoproduction of π 0 mesons off protons and neutrons in the second and third nucleon resonance regions

2018

Photoproduction of mesons off quasi-free nucleons bound in the deuteron allows to study the electromagnetic excitation spectrum of the neutron and the isospin structure of the excitation of nucleon resonances. The database for such reactions is much more sparse than for free proton targets. Single $\pi^0$ photoproduction off quasi-free nucleons from the deuteron was experimentally studied. Nuclear effects were investigated by a comparison of the results for free protons and quasi-free protons and used as a correction for the quasi-free neutron data. The experiment was performed at the tagged photon beam of the Mainz MAMI accelerator for photon energies between 0.45~GeV and 1.4~GeV, using an…

PhysicsNuclear reactionProtonMeson010308 nuclear & particles physicsHadronNuclear Theory7. Clean energy01 natural sciences3. Good healthNuclear physicsPionIsospin0103 physical sciencestagged photon spectrometer ; polarization observable E ; cross-sections ; pion-photoproduction ; baryon resonances ; deuteron ; MAMI ; asymmetry ; microtron ; thresholdNeutronddc:530010306 general physicsNucleonNuclear ExperimentNuclear Experiment
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Photoproduction of $ \pi^{0}$ -pairs off protons and off neutrons

2015

Total cross sections, angular distributions, and invariant-mass distributions have been measured for the photoproduction of $\pi^0\pi^0$ pairs off free protons and off nucleons bound in the deuteron. The experiments were performed at the MAMI accelerator facility in Mainz using the Glasgow photon tagging spectrometer and the Crystal Ball/TAPS detector. The accelerator delivered electron beams of 1508 and 1557~MeV, which produced bremsstrahlung in thin radiator foils. The tagged photon beam covered energies up to 1400~MeV. The data from the free proton target are in good agreement with previous measurements and were only used to test the analysis procedures. The results for differential cros…

Nuclear reactionPhysicsNuclear and High Energy PhysicsProtonMesonNuclear TheoryBremsstrahlung7. Clean energyDelta baryonNuclear physicsPhysics::Accelerator PhysicsNeutronAtomic physicsNuclear ExperimentNucleonNuclear ExperimentCrystal BallThe European Physical Journal A
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Measurement of the beam-helicity asymmetry in photoproduction of π0η pairs on carbon, aluminum, and lead

2020

The beam-helicity asymmetry was measured, for the first time, in photoproduction of $\pi^{0}\eta$ pairs on carbon, aluminum, and lead, with the A2 experimental setup at MAMI. The results are compared to an earlier measurement on a free proton and to the corresponding theoretical calculations. The Mainz model is used to predict the beam-helicity asymmetry for the nuclear targets. The present results indicate that the photoproduction mechanism for $\pi^{0}\eta$ pairs on nuclei is similar to photoproduction on a free nucleon. This process is dominated by the $D_{33}$ partial wave with the $\eta\Delta(1232)$ intermediate state.

Nuclear and High Energy PhysicsProtonmedia_common.quotation_subjectNuclear Theorychemistry.chemical_element7. Clean energy01 natural sciencesAsymmetryNuclear physicsAluminium0103 physical sciencesIntermediate stateNuclear Experiment010306 general physicsNuclear ExperimentQCmedia_commonPhysics010308 nuclear & particles physicsHelicitylcsh:QC1-9993. Good healthchemistryHigh Energy Physics::ExperimentNucleonCarbonlcsh:PhysicsBeam (structure)Physics Letters B
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Mechanisms in theC12(γ,pn)and(γ,pp)Reactions

1998

${}^{12}\mathrm{C}(\ensuremath{\gamma},pn)$ and $(\ensuremath{\gamma},pp)$ cross sections have been measured in kinematics which emphasize direct $2N$ knockout for ${E}_{\ensuremath{\gamma}}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}120--400\mathrm{MeV}$ and ${\ensuremath{\theta}}_{p}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}23\ifmmode^\circ\else\textdegree\fi{}--152\ifmmode^\circ\else\textdegree\fi{}$. The cross sections for both reactions peak strongly in the $\ensuremath{\Delta}$-resonance region. Theoretical calculations that account for the medium dependence of the $\ensuremath{\Delta}$ propagator predict a similar photon energy dependence to the data and describe the …

PhysicsGeneral Physics and AstronomyPropagatorAngular dependenceAtomic physicsPhoton energyPhysical Review Letters
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Quasifree photoproduction of eta mesons off protons and neutrons

2014

Differential and total cross sections for the quasifree reactions $\ensuremath{\gamma}p\ensuremath{\rightarrow}\ensuremath{\eta}p$ and $\ensuremath{\gamma}n\ensuremath{\rightarrow}\ensuremath{\eta}n$ have been determined at the MAMI-C electron accelerator by using a liquid deuterium target. Photons were produced via bremsstrahlung from the 1.5 GeV incident electron beam and energy tagged with the Glasgow photon tagger. Decay photons of the neutral decay modes $\ensuremath{\eta}\ensuremath{\rightarrow}2\ensuremath{\gamma}$ and $\ensuremath{\eta}\ensuremath{\rightarrow}3{\ensuremath{\pi}}^{0}\ensuremath{\rightarrow}6\ensuremath{\gamma}$ and coincident recoil nucleons were detected in a combin…

PhysicsNuclear and High Energy PhysicsParticle physicsNuclear TheoryProtonMesonNuclear TheoryBremsstrahlung7. Clean energyHigh Energy Physics - ExperimentNuclear physicsRecoilNeutronNuclear ExperimentNucleonNuclear ExperimentEnergy (signal processing)Crystal BallPHYSICAL REVIEW C
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Search for narrow dibaryon resonances in neutral pion photoproduction from the deuteron

2000

The reaction γd↦π0 X has been measured with TAPS at MAMI in the energy range E γ = 140-300 MeV. Using the Glasgow tagging spectrometer a photon energy resolution of 0.8 MeV was achieved. The energy excitation functions of integral and differential total cross-sections show no structures of statistical significance > 2σ. Upper limits for the production of narrow isoscalar or isovector dibaryons with masses m? 2100 MeV/c2 were deduced. They are in the range 2-5 μb averaged over the 0.8 MeV energy resolution.

PhysicsNuclear and High Energy PhysicsRange (particle radiation)Particle physicsIsovectorSpectrometer010308 nuclear & particles physicsIsoscalarNuclear TheoryHadronPhoton energy7. Clean energy01 natural sciencesNuclear physicsPion0103 physical sciencesNuclear fusionNuclear Experiment010306 general physicsThe European Physical Journal A
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Proton photoproduction from 12C

1995

Abstract The 12 C(γ,p) differential cross-section in the Δ-resonance region has been measured using tagged photons. Data are presented for 20 MeV wide photon energy bins at 200, 300, 400 and 500 MeV and for proton angles from 52° to 128°. The present 12 C(γ,p) measurements are compared with previous experiments carried out at Frascati, Tokyo and Bonn. Comparisons are also made with theoretical calculations developed at Gent and Valencia which provide an interpretation of the photon reaction mechanism in terms of the major contributing processes. Coincidence data with correlated neutrons, protons and pions are also presented.

PhysicsNuclear and High Energy PhysicsPhotonProtonbiologyNuclear TheoryPhoton energybiology.organism_classificationCoincidenceNuclear physicsPionNeutronNuclear ExperimentValenciaNuclear Physics A
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Coherent and incoherent π0 photoproduction from the deuteron

2001

Differential cross-sections for the reactions d(gamma,pi (o))d and d(gamma,pi (o))pn have been measured at MAMI with the TAPS detector setup in the energy range 140 MeV > E- > 306 MeV. By use of the Glasgow tagging spectrometer an 0.8 MeV energy resolution for photons incident on the target was achieved. The (o) missing energy resolution was sufficient for a reliable separation of coherent and incoherent channels. The data for the break-up channel exhibit very strong final state interaction effects, whereas the observed angular dependence of the inclusive process d(gamma, pi (o))X is in quantitative agreement with predictions for a quasi-free process. The observed absolute d(gamma, pi (o))X…

PhysicsNuclear and High Energy PhysicsRange (particle radiation)PhotonMissing energySpectrometer010308 nuclear & particles physicsHadron01 natural sciences7. Clean energyNuclear physicsDeuterium0103 physical sciencesNuclear fusionNeutronAtomic physicsNuclear Experiment010306 general physicsThe European Physical Journal A
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The12C(γ,NN)reaction studied over a wide kinematic range

2000

The ${}^{12}\mathrm{C}(\ensuremath{\gamma},np)$ and ${}^{12}\mathrm{C}(\ensuremath{\gamma},pp)$ reactions have been studied using the Glasgow photon tagging spectrometer at the Mainz MAMI electron microtron for ${E}_{\ensuremath{\gamma}}=150--700$ MeV over a kinematic range which extends well beyond the approximately back-to-back detector arrangements of previous work. For ${}^{12}\mathrm{C}(\ensuremath{\gamma},np)$ the general trends of the missing energy distributions are reproduced over a wide range of kinematics and photon energies by the theory developed by the Valencia group. The corresponding ${}^{12}\mathrm{C}(\ensuremath{\gamma},pp)$ channel is overestimated by a factor of \ensurem…

PhysicsNuclear physicsNuclear and High Energy PhysicsRange (particle radiation)RecoilMissing energyPhotonYield (chemistry)Monte Carlo methodResonanceElectronAtomic physicsNuclear ExperimentPhysical Review C
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In-medium modifications of the pi pi interaction in photon-induced reactions

2002

Differential cross sections of the reactions $(\gamma,\pi^\circ\pi^\circ)$ and $(\gamma,\pi^\circ\pi^++\pi^\circ\pi^-)$ have been measured for several nuclei ($^1$H,$^{12}$C, and $^{\rm nat}$Pb) at an incident-photon energy of $E_{\gamma}$=400-460 MeV at the tagged-photon facility at MAMI-B using the TAPS spectrometer. A significant nuclear-mass dependence of the $\pi\pi$ invariant-mass distribution is found in the $\pi^\circ\pi^\circ$ channel. This dependence is not observed in the $\pi^\circ\pi^{+/-}$ channel and is consistent with an in-medium modification of the $\pi\pi$ interaction in the $I$=$J$=0 channel. The data are compared to $\pi$-induced measurements and to calculations within …

PhysicsPhotonMesonPAIRSHadronCarbon-12General Physics and AstronomyElementary particleNONPERTURBATIVE APPROACHCHIRAL-SYMMETRY RESTORATIONPionNUCLEAR MEDIUMPiSPECTROMETERMESONAtomic physicsNuclear ExperimentNuclear ExperimentMATTERBoson
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Measurement of the beam-helicity asymmetry I⊙ in the photoproduction of π0-pairs off the proton and off the neutron

2013

Abstract Beam-helicity asymmetries have been measured at the MAMI accelerator in Mainz for the photoproduction of neutral pion pairs in the reactions γ → p → p π 0 π 0 and γ → d → ( n ) p π 0 π 0 , γ → d → ( p ) n π 0 π 0 off free protons and off quasi-free nucleons bound in the deuteron for incident photon energies up to 1.4 GeV. Circularly polarized photons were produced from bremsstrahlung of longitudinally polarized electrons and tagged with the Glasgow magnetic spectrometer. Decay photons from the π 0 mesons, recoil protons, and recoil neutrons were detected in the 4π covering electromagnetic calorimeter composed of the Crystal Ball and TAPS detectors. After kinematic reconstruction of…

PhysicsNuclear and High Energy PhysicsProtonMeson010308 nuclear & particles physicsNuclear TheoryHadron01 natural sciences7. Clean energyHelicityCharged particleNuclear physicsPion0103 physical sciencesHigh Energy Physics::ExperimentNeutronAtomic physicsNuclear Experiment010306 general physicsCrystal BallPhysics Letters B
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Neutron polarizabilities investigated by quasi-free Compton scattering from the deuteron

2002

Measuring Compton scattered photons and recoil neutrons in coincidence, quasifree Compton scattering by the neutron has been investigated at MAMI (Mainz) at ${\ensuremath{\theta}}_{\ensuremath{\gamma}}^{\mathrm{lab}}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}136\ifmmode^\circ\else\textdegree\fi{}$ in an energy range from 200 to 400 MeV. From the data a polarizability difference of ${\ensuremath{\alpha}}_{n}\ensuremath{-}{\ensuremath{\beta}}_{n}\phantom{\rule{0ex}{0ex}}=\phantom{\rule{0ex}{0ex}}9.8\ifmmode\pm\else\textpm\fi{}3.6(\mathrm{stat}{)}_{\ensuremath{-}1.1}^{+2.1}(\mathrm{syst})\ifmmode\pm\else\textpm\fi{}2.2(\mathrm{model})$ in units of ${10}^{\ensuremath{-}4}{\mathrm{fm}}^{…

Physics010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaCompton scatteringGeneral Physics and AstronomyFOS: Physical sciencesAstrophysics::Cosmology and Extragalactic Astrophysics7. Clean energy01 natural sciencesHigh Energy Physics - ExperimentHigh Energy Physics - PhenomenologyHigh Energy Physics - Experiment (hep-ex)High Energy Physics - Phenomenology (hep-ph)Deuterium0103 physical sciencesNeutronHigh Energy Physics::ExperimentAtomic physicsNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentEnergy (signal processing)Astrophysics::Galaxy Astrophysics
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First measurement of the helicity dependence of 3He photoreactions in the Δ(1232) resonance region

2013

The first measurement of the helicity dependence of the total inclusive 3He photo-absorption cross section and of the partial cross sections for several reaction channels was carried out at MAMI (Mainz) in the photon energy range between 150 and 500 MeV. The experiment used the large acceptance Crystal Ball spectrometer, complemented by charged particle and vertex detectors, a circularly polarised tagged photon beam and a longitudinally polarised high-pressure 3He gas target. The results obtained give information on the GDH integral on 3He and on the neutron and allow an investigation of the modifications of nucleon properties inside 3He.

PhysicsNuclear reactionNuclear and High Energy PhysicsPhoton010308 nuclear & particles physicsNuclear TheoryNucleon spin structurePhoton energy01 natural sciencesResonance (particle physics)HelicityNuclear physics0103 physical sciencesNeutronNuclear Experiment010306 general physicsCrystal BallPhysics Letters B
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K+Λ and K+Σ0 photoproduction with fine center-of-mass energy resolution

2014

Measurements of γp→K+Λγp→K+Λ and γp→K+Σ0γp→K+Σ0 cross-sections have been obtained with the photon tagging facility and the Crystal Ball calorimeter at MAMI-C. The measurement uses a novel K+K+ meson identification technique in which the weak decay products are characterized using the energy and timing characteristics of the energy deposit in the calorimeter, a method that has the potential to be applied at many other facilities. The fine center-of-mass energy (W) resolution and statistical accuracy of the new data results in a significant impact on partial wave analyses aiming to better establish the excitation spectrum of the nucleon. The new analyses disfavor a strong role for quark–diqua…

PhysicsNuclear and High Energy PhysicsPhotonMesonResolution (electron density)7. Clean energyCalorimeterNuclear physicsHigh Energy Physics::ExperimentCenter of massAtomic physicsNucleonExcitationCrystal BallPhysics Letters B
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The selection and performance of diamond radiators used in coherent bremsstrahlung experiments

2005

The bremsstrahlung emitted as a result of scattering electrons in thin diamond crystals provides a useful source of high energy photons for use in photonuclear experiments, since the coherent bremsstrahlung produced is linearly polarized. Techniques for selecting the most favorable diamonds have been investigated. These are optical polaroid analysis, X-ray topography and rocking curve measurements. The diamonds are characterized with a view to determining their performance as radiators, and bremsstrahlung spectra from a diamond radiator used at the Mainz MAMI-B facility are presented. The changes caused by high energy electrons to the crystal properties of the diamond and to the resulting c…

PhysicsNuclear and High Energy PhysicsHigh energybusiness.industryScatteringLinear polarizationAstrophysics::High Energy Astrophysical PhenomenaBremsstrahlungDiamondElectronengineering.materialSpectral lineOpticsRadiator (engine cooling)engineeringAtomic physicsNuclear ExperimentbusinessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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Incoherent neutral pion photoproduction on 12C.

2007

We present the first detailed measurement of incoherent photoproduction of neutral pions to a discrete state of a residual nucleus. The C-12(gamma,pi(0))C-12(4.4 MeV)* reaction has been studied with the Glasgow photon tagger at MAMI employing a new technique which uses the large solid angle Crystal Ball detector both as a pi(0) spectrometer and to detect decay photons from the excited residual nucleus. The technique has potential applications to a broad range of future nuclear measurements with the Crystal Ball and similar detector systems elsewhere. Such data are sensitive to the propagation of the Delta in the nuclear medium and will give the first information on matter transition form fa…

PhysicsNuclear reactionPhotonMesonmeasurement of incoherent photoproduction010308 nuclear & particles physicsHadronNuclear TheoryGeneral Physics and AstronomyElementary particle01 natural sciences7. Clean energyNuclear physicsPionExcited state0103 physical sciencesAtomic physics010306 general physicsNuclear ExperimentCrystal BallPhysical review letters
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Low-energy Compton scattering and the polarizabilities of the proton

2001

Differential cross-sections for Compton scattering from the proton have been measured at the MAMI tagged photon facility using the TAPS setup. The data cover an angular range of θlab γ = 59°-155° and photon energies ranging from 55 MeV to 165 MeV. Our results are in good agreement with those from previous experiments, but yield higher precision. Using dispersion relations the proton polarizabilities have been determined to be = [11.9±0.5stat.±1.3syst.±0.3mod.] . 10-4 fm 3 and = [1.2±0.7stat.±0.3syst.±0.4mod.)] . 10-4 fm 3. These results confirm the Baldin sum rule which was re-evaluated to be + = [13.8±0.4] . 10-4 fm 3. We can also conclude that there is no significant additional asymptotic…

PhysicsNuclear and High Energy PhysicsPhotonProton010308 nuclear & particles physicsHadronCompton scattering01 natural sciencesNuclear physicsPolarizabilityDispersion relation0103 physical sciencesSum rule in quantum mechanicsAtomic physics010306 general physicsSpin-½The European Physical Journal A
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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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Angular distribution of coherent bremsstrahlung

2012

The angular distribution of the linearly polarised photon beam produced by coherent bremsstrahlung from an aligned diamond radiator has been measured at the MAMI A2 tagged photon facility. The measurements were made with a prototype position sensitive photon detector which utilises the pair production process and a double sided silicon strip detector. This polarised photon beam is used for nuclear and hadronic experiments and in their analysis the polarisation is obtained from a calculation, which matches the experimental intensity spectrum. As the polarisation is related to the photon beam angular distribution, the present measurements can be used to test this calculation. The overall agre…

PhysicsNuclear and High Energy PhysicsPhotonbusiness.industryDetectorHadronBremsstrahlungDiamondengineering.materialOpticsPair productionPosition (vector)engineeringRadiator (engine cooling)businessInstrumentationNuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
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12C(γ,π+n) and 12C(γ,π+p) reactions across the Δ resonance region

1997

Abstract Differential cross-sections from (γ,π+n) and (γ,π+p) experiments on 12C are presented together with a microscopic model calculation. The comparison of experimental data with theory confirms that quasifree pion production is the dominant process for the (γ,π+n) reaction. The comparison of (γ,π+p) with (γ,π+n) data shows the importance of final state interactions. first time to experimentally study the strength and the possible mechanisms involved in the final state interaction.

PhysicsNuclear and High Energy PhysicsCrystallographyPionAtomic physicsResonance (chemistry)Physics Letters B
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Three-nucleon mechanisms in photoreactions

2002

The $^{12}$C$(\gamma,ppn)$ reaction has been measured for E$_{\gamma}$=150-800 MeV in the first study of this reaction in a target heavier than $^3$He. The experimental data are compared to a microscopic many body calculation. The model, which predicts that the largest contribution to the reaction arises from final state interactions following an initial pion production process, overestimates the measured cross sections and there are strong indications that the overestimate arises in this two-step process. The selection of suitable kinematic conditions strongly suppresses this two-step contribution leaving cross sections in which up to half the yield is predicted to arise from the absorptio…

Nuclear physicsPhysicsNuclear and High Energy PhysicsPhotonPionYield (chemistry)FOS: Physical sciencesAbsorption (logic)Nuclear Experiment (nucl-ex)NucleonNuclear ExperimentNuclear ExperimentMany body
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Measurement of the Gerasimov-Drell-Hearn Integrand forH2from 200 to 800 MeV

2006

A measurement of the helicity dependence of the total inclusive photoabsorption cross section on the deuteron was carried out at MAMI (Mainz) in the energy range $200l{E}_{\ensuremath{\gamma}}l800\text{ }\text{ }\mathrm{MeV}$. The experiment used a $4\ensuremath{\pi}$ detection system, a circularly polarized tagged photon beam and a frozen-spin target which provided longitudinally polarized deuterons. The contribution to the Gerasimov-Drell-Hearn sum rule for the deuteron determined from the data is $407\ifmmode\pm\else\textpm\fi{}20(\mathrm{stat})\ifmmode\pm\else\textpm\fi{}24(\mathrm{syst})\text{ }\text{ }\ensuremath{\mu}\mathrm{b}$ for $200l{E}_{\ensuremath{\gamma}}l800\text{ }\text{ }\m…

PhysicsParticle physicsMeson production010308 nuclear & particles physicsNuclear TheoryGeneral Physics and AstronomyComputer Science::Computation and Language (Computational Linguistics and Natural Language and Speech Processing)01 natural sciencesHelicityNuclear physics0103 physical sciencesSum rule in quantum mechanicsPhoton beamNuclear Experiment010306 general physicsEnergy (signal processing)Physical Review Letters
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Study of η and η′ Photoproduction at MAMI

2017

The reactions γp→ηp and γp→η′p are measured from their thresholds up to the center-of-mass energy W=1.96  GeV with the tagged-photon facilities at the Mainz Microtron, MAMI. Differential cross sections are obtained with unprecedented statistical accuracy, providing fine energy binning and full production-angle coverage. A strong cusp is observed in the total cross section for η photoproduction at the energies in the vicinity of the η′ threshold, W=1896  MeV (Eγ=1447  MeV). Within the framework of a revised ηMAID isobar model, the cusp, in connection with a steep rise of the η′ total cross section from its threshold, can only be explained by a strong coupling of the poorly known N(1895)1/2− …

Cusp (singularity)PhysicsParticle physicsPhotonProton010308 nuclear & particles physicsGeneral Physics and Astronomy01 natural sciencesNuclear physicsCross section (physics)Excited state0103 physical sciencesIsobar010306 general physicsMicrotronCrystal BallPhysical Review Letters
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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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Nuclear pion photoproduction in theΔresonance region

1999

A measurement of the /sup 12/C( gamma , pi /sup +/n)/sup 11/B reaction in quasifree pi -production kinematic regimes has been performed using tagged photons in conjunction with large solid angle pi and n detectors. The aim of the experiment was to investigate predicted modifications to the Delta excitation of nucleons and their subsequent propagation and decay, brought about by the nuclear medium. Differential cross sections are presented for photon energies spanning the Delta (1232) excitation region. The measurements are consistent with distorted wave impulse approximation calculations in which the amplitude for proton Delta excitation, followed by Delta propagation and decay to pi /sup +…

Nuclear physicsPhysicsDeltaNuclear and High Energy PhysicsPionAmplitudePhotonSolid angleImpulse (physics)Atomic physicsNucleonExcitationPhysical Review C
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Helicity dependence of the total inclusive cross section on the deuteron

2009

Abstract A measurement of the helicity dependence of the total inclusive photoabsorption cross section on the deuteron was carried out at MAMI (Mainz) in the energy range 200 E γ 800 MeV . The experiment used a 4 π detection system, a circularly polarized tagged photon beam and a frozen spin target which provided longitudinally polarized deuterons. These new results are a significant improvement on the existing data and allow a detailed comparison with state-of-the-art calculations.

PhysicsAngular momentumRange (particle radiation)Nuclear and High Energy PhysicsNuclear TheoryPolarization (waves)HelicityDeuteron photoabsorptionCharged particleNuclear physicsCross section (physics)DeuteriumPhysics and AstronomyDouble polarization experimentSpin (physics)Nuclear ExperimentPhysics Letters B
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Measurement of the π0→e+e−γ Dalitz decay at the Mainz Microtron

2017

The Dalitz decay π0→e+e−γ has been measured in the γp→π0p reaction with the A2 tagged-photon facility at the Mainz Microtron, MAMI. The value obtained for the slope parameter of the π0 electromagnetic transition form factor, aπ=0.030±0.010tot, is in agreement with existing measurements of this decay and with recent theoretical calculations. The uncertainty obtained in the value of aπ is lower than in previous results based on the π0→e+e−γ decay.

Nuclear physicsPhysicsParticle physicsMeson010308 nuclear & particles physics0103 physical sciencesForm factor (quantum field theory)010306 general physics01 natural sciencesMicrotronDark photonPhysical Review C
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Backward spin polarizabilityγπof the proton

2002

Using the Mainz $48\mathrm{cm}\ensuremath{\emptyset}\ifmmode\times\else\texttimes\fi{}64\mathrm{cm}$ NaI(Tl) detector and the segmented G\"ottingen recoil detector SENECA in coincidence, Compton scattering by the proton at ${\ensuremath{\theta}}_{\ensuremath{\gamma}}^{\mathrm{lab}}=136\ifmmode^\circ\else\textdegree\fi{}$ has been measured at MAMI (Mainz) in the energy range from 200 to 470 MeV. The new data confirm the previous observation that there is a systematic discrepancy between MAMI and LEGS (Brookhaven) data leading to different spin polarizabilities ${\ensuremath{\gamma}}_{\ensuremath{\pi}}=\ensuremath{-}38.7\ifmmode\pm\else\textpm\fi{}1.8$ and $\ensuremath{-}27.2\ifmmode\pm\else\…

Elastic scatteringPhysicsNuclear and High Energy PhysicsParticle physicsProton010308 nuclear & particles physicsHadronElementary particle01 natural sciencesOrientation (vector space)Nuclear physicsBaryon0103 physical sciences010306 general physicsNucleonEnergy (signal processing)Physical Review C
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Differential cross section for the reaction 2H(γ, p)n from 133 to 158 MeV

1991

The cross section for the reaction 2H(γ, p)n has been measured at laboratory photon energies Eγ = 133−158 MeV and c.m. angles between 30° and 150°. The reaction was induced by a tagged bremsstrahlung photon beam incident on a liquid deuterium target. The uncertainty in the absolute cross sections is ⩽ 5%. There is now reasonable agreement between recent measurements in this energy region and the overall data set now defines the cross section sufficiently well to provide a test of current models of the reaction.

Scattering cross-sectionNuclear reactionPhysicsNuclear physicsNuclear and High Energy PhysicsCross section (physics)PhotonDeuteriumNuclear cross sectionAtomic physicsBeam (structure)Bremsstrahlung photonNuclear Physics A
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Measurement of theH1(γ⃗, p⃗)π0Reaction Using a Novel Nucleon Spin Polarimeter

2014

We report the first large-acceptance measurement of polarization transfer from a polarized photon beam to a recoiling nucleon. The measurement pioneers a novel polarimetry technique, which can be applied to many other nuclear and hadron physics experiments. The commissioning reaction of $^{1}H(\mathrm{\ensuremath{\gamma}P\vec},\text{ }\mathrm{pP\vec}){\ensuremath{\pi}}^{0}$ in the range $0.4l{E}_{\ensuremath{\gamma}}l1.4\text{ }\text{ }\mathrm{GeV}$ validates the technique and provides essential new data to constrain the excitation spectrum of the nucleon.

PhysicsParticle physicsMeson productionPartial wave analysisNuclear TheoryGeneral Physics and AstronomyPolarimeterPolarization (waves)7. Clean energyNuclear physicsHadron physicsPhoton beamNuclear ExperimentNucleonExcitationPhysical Review Letters
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Photoproduction ofπ0Mesons off Neutrons in the Nucleon Resonance Region

2014

Precise angular distributions have been measured for the first time for the photoproduction of π0 mesons off neutrons bound in the deuteron. The effects from nuclear Fermi motion have been eliminated by a complete kinematic reconstruction of the final state. The influence of final-state-interaction effects has been estimated by a comparison of the reaction cross section for quasifree protons bound in the deuteron to the results for free protons and then applied as a correction to the quasifree neutron data. The experiment was performed at the tagged photon facility of the Mainz Microtron MAMI with the Crystal Ball and TAPS detector setup for incident photon energies between 0.45 and 1.4 GeV…

PhysicsParticle physicsMesonProtonNuclear TheoryGeneral Physics and AstronomyPhoton energy7. Clean energyNuclear physicsIsospinNeutronNuclear ExperimentNucleonMicrotronCrystal BallPhysical Review Letters
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First measurement of the circular beam asymmetry in the γ→p→π0ηp reaction

2010

Abstract The circular photon asymmetry for π 0 η photoproduction on the proton was measured for the first time at the tagged photon facility of the MAMI C accelerator using the Crystal Ball/TAPS photon spectrometer. The experimental results are interpreted within a phenomenological isobar model that confirms the dominant role of the Δ ( 1700 ) D 33 resonance. The measured asymmetry allows us to identify small contributions from positive-parity resonances via interference terms with the dominant D 33 amplitude.

PhysicsNuclear reactionNuclear and High Energy PhysicsPhotonProton010308 nuclear & particles physicsmedia_common.quotation_subjectResonanceElementary particle01 natural sciencesAsymmetryDelta baryonNuclear physics0103 physical sciencesNuclear Experiment010306 general physicsCrystal Ballmedia_commonPhysics Letters B
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Scaling of the 4He(γ,p)t reaction in the Eγ = 80–160 MeV region

1993

The 4He(γ,p) 3H reaction cross section has been measured with tagged photons of energy 81–158 MeV. Protons were detected over the angular range 55°–125°. The scaling of the data as a function of momentum mismatch has been examined for two reaction models, the modified quasideuteron mechanism and quasifree knockout. Both models show clear scaling behaviour but comparison of the predicted and measured scaling function shapes favours the modified quasideuteron mechanism at momenta up to ≈500 MeV/c.

PhysicsMomentumNuclear physicsNuclear and High Energy PhysicsCross section (physics)Angular rangePhotonReaction modelNuclear TheoryAtomic physicsNuclear ExperimentScalingPhysics Letters B
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Helicity Dependence ofγp→Nπbelow 450 MeV and Contribution to the Gerasimov-Drell-Hearn Sum Rule

2000

The helicity dependence of the single pion photoproduction on the proton has been measured in the energy range from 200 to 450 MeV for the first time. The experiment, performed at the Mainz microtron MAMI, used a 4pi-detector system, a circularly polarized, tagged photon beam, and a frozen-spin target. The data obtained provide new information for multipole analyses of pion photoproduction and determine the main contributions to the Gerasimov-Drell-Hearn sum rule and the forward spin polarizability gamma(0).

PhysicsParticle physicsProtonNuclear TheoryGeneral Physics and AstronomyHelicityNuclear physicsPionPolarizabilityPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentSum rule in quantum mechanicsNuclear ExperimentMultipole expansionMicrotronSpin-½Physical Review Letters
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Narrow Structure in the Excitation Function of eta Photoproduction off the Neutron

2013

The photoproduction of $\eta$-mesons off nucleons bound in $^2$H and $^3$He has been measured in coincidence with recoil protons and recoil neutrons for incident photon energies from threshold up to 1.4 GeV. The experiments were performed at the Mainz MAMI accelerator, using the Glasgow tagged photon facility. Decay photons from the $\eta\rightarrow 2\gamma$ and $\eta\rightarrow 3\pi^0$ decays and the recoil nucleons were detected with an almost $4\pi$ electromagnetic calorimeter combining the Crystal Ball and TAPS detectors. The data from both targets are of excellent statistical quality and show a narrow structure in the excitation function of $\gamma n\rightarrow n\eta$. The results from…

ProtonMesonNuclear TheoryFOS: Physical sciencesGeneral Physics and AstronomyPhysics::OpticsPhoton energyη; meson; photoproduction off the neutron; MAMI01 natural sciences7. Clean energyNuclear physicsRecoil0103 physical sciencesNeutronNuclear Experiment (nucl-ex)010306 general physicsNuclear ExperimentNuclear ExperimentPhysicsExcitation function010308 nuclear & particles physicsPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentAtomic physicsNucleonCrystal BallPHYSICAL REVIEW LETTERS
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Polarized photon measurements of the12C(γ→,pp)and12C(γ→,pn)reactions forEγ=160−350MeV

2001

The ${}^{12}\mathrm{C}(\stackrel{\ensuremath{\rightarrow}}{\ensuremath{\gamma}},pp)$ and ${}^{12}\mathrm{C}(\stackrel{\ensuremath{\rightarrow}}{\ensuremath{\gamma}},pn)$ reactions have been studied for ${E}_{\ensuremath{\gamma}}=160\ensuremath{-}350$ MeV using linearly polarized photons from the Glasgow tagged photon spectrometer at the Mainz microtron MAMI. Both reaction channels show a negative photon asymmetry $\ensuremath{\Sigma}$ for missing energies ${E}_{m}$ below 70 MeV, where direct emission nucleon pairs is expected. A strong peak at low ${E}_{m}$ is observed in ${\ensuremath{\Sigma}}_{(\ensuremath{\gamma},pp)},$ but not in ${\ensuremath{\Sigma}}_{(\ensuremath{\gamma},pn)}.$ Furth…

PhysicsNuclear and High Energy PhysicsPhotonPionmedia_common.quotation_subjectNuclear TheoryProduction (computer science)Angular dependenceAtomic physicsNuclear ExperimentNucleonAsymmetrymedia_commonPhysical Review C
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C12(γ,p)11B cross section from 80 to 157 MeV

1995

The $^{12}\mathrm{C}$(\ensuremath{\gamma},p${)}^{11}$B differential cross section has been measured over proton angles ranging from 58\ifmmode^\circ\else\textdegree\fi{} to 128\ifmmode^\circ\else\textdegree\fi{}, using tagged photons of energy 80--157 MeV, for low-lying regions of residual excitation energy in $^{11}\mathrm{B}$. The data have been compared with four different types of calculation. It is shown that scaling of the cross section with momentum mismatch occurs for both the ground-state and excited-state data.

Nuclear reactionPhysicsBaryonNuclear and High Energy PhysicsProtonHadronElementary particleIsotopes of boronAtomic physicsNucleonEnergy (signal processing)Physical Review C
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The Reactionγp→π0γ′pand the Magnetic Dipole Moment of theΔ+(1232)Resonance

2002

The reaction $\ensuremath{\gamma}p\ensuremath{\rightarrow}{\ensuremath{\pi}}^{0}{\ensuremath{\gamma}}^{\ensuremath{'}}p$ has been measured with the TAPS calorimeter at the Mainz Microtron accelerator facility MAMI for energies between $\sqrt{s}=1221--1331\text{ }\text{ }\mathrm{M}\mathrm{e}\mathrm{V}$. The cross section's differential in angle and energy have been determined for the photon ${\ensuremath{\gamma}}^{\ensuremath{'}}$ in three bins of the excitation energy. This reaction channel provides access to the magnetic dipole moment of the ${\ensuremath{\Delta}}^{+}(1232)$ resonance and, for the first time, a value of ${\ensuremath{\mu}}_{{\ensuremath{\Delta}}^{+}}=\mathbf{[}{2.7}_{\ensu…

BaryonPhysicsCrystallographyParticle physicsAngular distributionMagnetic momentPiGeneral Physics and AstronomyResonanceNuclear ExperimentEnergy (signal processing)Physical Review Letters
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Photoproduction of π0-pairs off protons and off neutrons

2015

Total cross sections, angular distributions, and invariant-mass distributions have been measured for the photoproduction of π0π0 pairs off free protons and off nucleons bound in the deuteron. The experiments were performed at the MAMI accelerator facility in Mainz using the Glasgow photon tagging spectrometer and the Crystal Ball/TAPS detector. The accelerator delivered electron beams of 1508 and 1557MeV, which produced bremsstrahlung in thin radiator foils. The tagged photon beam covered energies up to 1400MeV. The data from the free proton target are in good agreement with previous measurements and were only used to test the analysis procedures. The results for differential cross sections…

Nuclear TheoryNuclear Experiment
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Measurement of the $^{1}H$($\vec{\gamma}$, $\vec{p}$)$\pi^{0}$ reaction using a novel nucleon spin polarimeter

2013

We report the first large-acceptance measurement of polarization transfer from a polarized photon beam to a recoiling nucleon, pioneering a novel polarimetry technique with wide application to future nuclear and hadronic physics experiments. The commissioning measurement of polarization transfer in the $^{1}H$($\vec{\gamma}$,$\vec{p}$)$\pi^{0}$ reaction in the range $0.4<E_{\gamma}<1.4$ GeV is highly selective regarding the basic parameterizations used in partial wave analyses to extract the nucleon excitation spectrum. The new data strongly favor the recently proposed Chew-Mandelstam formalism.

Nuclear TheoryNuclear ExperimentNuclear Experiment
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Study of $\eta$ and $\eta'$ photoproduction at MAMI

2017

The reactions $\gamma p\to \eta p$ and $\gamma p\to \eta' p$ have been measured from their thresholds up to the center-of-mass energy $W=1.96$GeV with the tagged-photon facilities at the Mainz Microtron, MAMI. Differential cross sections were obtained with unprecedented accuracy, providing fine energy binning and full production-angle coverage. A strong cusp is observed in the total cross section and excitation functions for $\eta$ photoproduction at the energies in vicinity of the $\eta'$ threshold, $W=1896$MeV ($E_\gamma=1447$MeV). This behavior is explained in a revised $\eta$MAID isobar model by a significant branching of the $N(1895)1/2^-$ nucleon resonance to both, $\eta p$ and $\eta'…

High Energy Physics - PhenomenologyNuclear TheoryHigh Energy Physics::ExperimentNuclear ExperimentNuclear ExperimentHigh Energy Physics - Experiment
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Study of eta and eta' Photoproduction at MAMI

2017

The reactions γp→ηp and γp→η′p are measured from their thresholds up to the center-of-mass energy W=1.96 GeV with the tagged-photon facilities at the Mainz Microtron, MAMI. Differential cross sections are obtained with unprecedented statistical accuracy, providing fine energy binning and full production-angle coverage. A strong cusp is observed in the total cross section for η photoproduction at the energies in the vicinity of the η′ threshold, W=1896 MeV (Eγ=1447 MeV). Within the framework of a revised ηMAID isobar model, the cusp, in connection with a steep rise of the η′ total cross section from its threshold, can only be explained by a strong coupling of the poorly known N(1895)1/2− sta…

spectrometer ; photons ; proton ; taps
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