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N{yields}{Delta} transition and proton polarizabilities from measurements of p({rvec {gamma}},{gamma}), p({rvec {gamma}},{pi}{sup 0}), and p({rvec {gamma}},{pi}{sup +})

Journal Article · · Physical Review C

We report new high-precision measurements of p({rvec {gamma}},{gamma}), p({rvec {gamma}},{pi}{sup 0}) and p({rvec {gamma}},{pi}{sup +}) cross section and beam asymmetry angular distributions for photon beam energies in the range from 213 MeV to 333 MeV. The cross sections for all three channels are locked together with a small common systematic scale uncertainty of 2%. A large overdetermination of kinematic parameters was used to achieve the first complete separation of the Compton scattering and {pi}{sup 0}-production channels. This has also allowed all detector efficiencies for the p({rvec {gamma}},{gamma}) and p({rvec {gamma}},{pi}{sup 0}) channels to be measured directly from the data itself without resorting to simulations. The new Compton results are approximately 30% higher than previous Bonn data near the peak of the {Delta} resonance, resolving a long-standing unitarity puzzle. However, our p({rvec {gamma}},{pi}{sup 0}) and p({rvec {gamma}},{pi}{sup +}) cross sections are also about 10% higher than both earlier Bonn data and recent Mainz measurements, while our p({rvec {gamma}},{pi}{sup +}) cross sections are in good agreement with results from Tokyo. Our polarization asymmetry data are of the highest precision yet available and have considerable impact upon multipole analyses. These new data have been combined with other polarization ratios in a simultaneous analysis of both Compton scattering and {pi} production, with Compton scattering providing two new constraints on the photopion amplitude. This analysis has improved the accuracy in the E2/M1 mixing ratio for the N{yields}{Delta} transition, EMR=-[3.07{+-}0.26(stat+syst){+-}0.24(model)](%), and the corresponding N{yields}{Delta} transverse helicity amplitudes, A{sub 1/2}=-[135.7{+-}1.3(stat+syst){+-}3.7(model)](10{sup -3}GeV{sup -1/2}) and A{sub 3/2}=-[266.9{+-}1.6(stat+syst){+-}7.8(model)](10{sup -3}GeV{sup -1/2}). From these we deduce an oblate spectroscopic deformation for the {Delta}{sup +}. The same simultaneous analysis has been used to extract the proton dipole polarizabilities, {bar {alpha}}-{bar {beta}}=+[10.39{+-}1.77(stat+syst){sub -1.87}{sup +1.02}(model)](10{sup -4}fm{sup 3}) in agreement with previous low energy measurements, and {bar {alpha}}+{bar {beta}}=+[13.25{+-}0.86(stat+syst){sub -0.58}{sup +0.23}(model)](10{sup -4}fm{sup 3}) in agreement with recent evaluations of the Baldin sum rule. Our simultaneous analysis has also provided the first determination of the proton spin polarizabilities, {gamma}{sub {pi}}=-[27.23{+-}2.27(stat+syst){sub -2.10}{sup +2.24}(model)](10{sup -4}fm{sup 4}), {gamma}{sub 0}=-[1.55{+-}0.15(stat+syst){sub -0.03}{sup +0.03}(model)](10{sup -4}fm{sup 4}), {gamma}{sub 13}=+[3.94{+-}0.53(stat+syst){sub -0.18}{sup +0.20}(model)](10{sup -4}fm{sup 4}), and {gamma}{sub 14}=-[2.20{+-}0.27(stat+syst){sub -0.09}{sup +0.05}(model)](10{sup -4}fm{sup 4}). The extracted value of the backward spin polarizability, {gamma}{sub {pi}}, is considerably different from other analyses and this has been instrumental in bringing the value of {bar {alpha}}-{bar {beta}} extracted from high energy data into agreement with low energy experiments.

Research Organization:
Brookhaven National Laboratory
Sponsoring Organization:
(US)
DOE Contract Number:
AC02-98CH10886
OSTI ID:
40277003
Journal Information:
Physical Review C, Journal Name: Physical Review C Journal Issue: 2 Vol. 64; ISSN 0556-2813
Publisher:
The American Physical Society
Country of Publication:
United States
Language:
English

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