378 research outputs found

    Measurements of the Generalized Electric and Magnetic Polarizabilities of the Proton at Low Q2 Using the VCS Reaction

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    The mean square polarizability radii of the proton have been measured for the first time in a virtual Compton scattering experiment performed at the MIT-Bates out-of-plane scattering facility. Response functions and polarizabilities obtained from a dispersion analysis of the data at Q2=0.06 GeV2/c2 are in agreement with O(p3) heavy baryon chiral perturbation theory. The data support the dominance of mesonic effects in the polarizabilities, and the increase of beta with increasing Q2 is evidence for the cancellation of long-range diamagnetism by short-range paramagnetism from the pion cloud

    Measurement of the Partial Cross Sections s(TT), s(LT) and [s(T)+epsilon*s(L)] of the p(e,e' pi+)n Reaction in the Delta(1232) Resonance

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    We report new precision p(e,e' pi+})n measurements in the Delta(1232) resonance at Q2 = 0.127(GeV/c)2 obtained at the MIT-Bates Out-Of-Plane scattering facility. These are the lowest, but non-zero, Q2 measurements in the pi+ channel. The data offer new tests of the theoretical calculations, particularly of the background amplitude contributions. The chiral effective field theory and Sato-Lee model calculations are not in agreement with this experiment

    Investigation of the conjectured nucleon deformation at low momentum transfer

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    We report new precise H(e,ep)π0(e,e^\prime p)\pi^0 measurements at the Δ(1232)\Delta(1232) resonance at Q2=0.127Q^2= 0.127 (GeV/c)2^2 using the MIT/Bates out-of-plane scattering (OOPS) facility. The data reported here are particularly sensitive to the transverse electric amplitude (E2E2) of the γNΔ\gamma^* N\to\Delta transition. Analyzed together with previous data yield precise quadrupole to dipole amplitude ratios EMR=(2.3±0.3stat+sys±0.6model)EMR = (-2.3 \pm 0.3_{stat+sys} \pm 0.6_{model})% and CMR=(6.1±0.2stat+sys±0.5model)CMR = (-6.1 \pm 0.2_{stat+sys}\pm 0.5_{model})% and for M1+3/2=(41.4±0.3stat+sys±0.4model)(103/mπ+)M^{3/2}_{1+} = (41.4 \pm 0.3_{stat+sys}\pm 0.4_{model})(10^{-3}/m_{\pi^+}). They give credence to the conjecture of deformation in hadronic systems favoring, at low Q2Q^2, the dominance of mesonic effects.Comment: 4 pages, 1figur

    Threshold Electrodisintegration of ^3He

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    Cross sections were measured for the near-threshold electrodisintegration of ^3He at momentum transfer values of q=2.4, 4.4, and 4.7 fm^{-1}. From these and prior measurements the transverse and longitudinal response functions R_T and R_L were deduced. Comparisons are made against previously published and new non-relativistic A=3 calculations using the best available NN potentials. In general, for q<2 fm^{-1} these calculations accurately predict the threshold electrodisintegration of ^3He. Agreement at increasing q demands consideration of two-body terms, but discrepancies still appear at the highest momentum transfers probed, perhaps due to the neglect of relativistic dynamics, or to the underestimation of high-momentum wave-function components.Comment: 9 pages, 7 figures, 1 table, REVTEX4, submitted to Physical Review

    A New Measurement of the π0\pi^0 Radiative Decay Width

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    High precision measurements of the differential cross sections for π0\pi^0 photoproduction at forward angles for two nuclei, 12^{12}C and 208^{208}Pb, have been performed for incident photon energies of 4.9 - 5.5 GeV to extract the π0γγ{\pi^0 \to \gamma\gamma} decay width. The experiment was done at Jefferson Lab using the Hall B photon tagger and a high-resolution multichannel calorimeter. The π0γγ{\pi^0 \to \gamma\gamma} decay width was extracted by fitting the measured cross sections using recently updated theoretical models for the process. The resulting value for the decay width is Γ(π0γγ)=7.82±0.14 (stat.)±0.17 (syst.) eV\Gamma{(\pi^0 \to \gamma\gamma)} = 7.82 \pm 0.14 ~({\rm stat.}) \pm 0.17 ~({\rm syst.}) ~{\rm eV}. With the 2.8% total uncertainty, this result is a factor of 2.5 more precise than the current PDG average of this fundamental quantity and it is consistent with current theoretical predictions.Comment: 4 pages, 5 figure

    Measurement of the beam-helicity asymmetry in photoproduction of π0η pairs on carbon, aluminum, and lead

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    The beam-helicity asymmetry was measured, for the first time, in photoproduction of π0η\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 π0η\pi^{0}\eta pairs on nuclei is similar to photoproduction on a free nucleon. This process is dominated by the D33D_{33} partial wave with the ηΔ(1232)\eta\Delta(1232) intermediate state

    Measurement of the transverse target and beam-target asymmetries in η\eta meson photoproduction at MAMI

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    We present new data for the transverse target asymmetry T and the very first data for the beam-target asymmetry F in the γpηp\vec \gamma \vec p\to\eta p reaction up to a center-of-mass energy of W=1.9 GeV. The data were obtained with the Crystal-Ball/TAPS detector setup at the Glasgow tagged photon facility of the Mainz Microtron MAMI. All existing model predictions fail to reproduce the new data indicating a significant impact on our understanding of the underlying dynamics of η\eta meson photoproduction. The peculiar nodal structure observed in existing T data close to threshold is not confirmed.Comment: 5 pages, 3 figures, accepted for publication in PR
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