6533b7d4fe1ef96bd1261fbd
RESEARCH PRODUCT
Compton Scattering by the Proton
S. ProffR. KondratievR. BeckS.j. HallF. HärterA. RobbianoC. MolinariG. GallerP. OttonelloA.i. L'vovM. SchmitzM. CamenP. JenneweinF. WissmannMartin SchumacherI. PreobrajenskiG. P. CapitaniJ. PeiseAnna Maria MassoneP. GrabmayrV. LisinS. WolfT. HehlH.-j. ArendsJ. AhrensM. SanzoneK. Kossertsubject
PhysicsNuclear and High Energy PhysicsPhotonProton010308 nuclear & particles physicsNuclear TheoryCompton scatteringFOS: Physical sciences7. Clean energy01 natural sciencesResonance (particle physics)Scattering amplitudeNuclear physicsHigh Energy Physics - PhenomenologyHigh Energy Physics - Phenomenology (hep-ph)Polarizability0103 physical sciencesPhysics::Accelerator PhysicsHigh Energy Physics::ExperimentNuclear Experiment (nucl-ex)010306 general physicsMultipole expansionNuclear ExperimentNuclear ExperimentSpin-½description
Compton scattering by the proton has been measured over a wide range covering photon energies 250 MeV < E_\gamma < 800 MeV and photon scattering angles 30^0 < \theta^{lab}_\gamma < 150^0, using the tagged-photon facility at MAMI (Mainz) and the large-acceptance arrangement LARA. The data are in good agreement with the dispersion theory based on the SAID-SM99K parameterization of photo-meson amplitudes. From the subset of data between 280 and 360 MeV the resonance pion-photoproduction amplitudes were evaluated leading to the multipole E2/M1 ratio EMR(340 MeV) =(-1.6 \pm 0.4(stat+syst) \pm 0.2(model)%. From all data below 455 MeV the proton's backward spin polarizability was determined to be \gamma_\pi=(-37.9 \pm 0.6(stat+syst) \pm 3.5(model))x10^{-4}fm^4.
year | journal | country | edition | language |
---|---|---|---|---|
2001-02-06 |