6533b7d2fe1ef96bd125f805
RESEARCH PRODUCT
Compton scattering from the free and bound proton at backward angles above π-threshold
M. KotullaB. KruscheE. HeidR. W. NovotnyK. KossertV. MetagD. RosenkranzF. RamboAnthony W. ThomasG. CaselottiF. ZapadtkaM. CamenH. VorwerkR. BeckI. PreobrashenskijJ. AhrensP. AchenbachR. KondratjevJ. WeissH. StröherTh. WalcherA. SchmidtF. WissmannB. SeitzU. SiodlaczekR. LeukelO. JahnA. PolonskiV. Olmos De LeónM.i. LevchukV. KuhrP. JenneweinMatthias WolfV. LisinE. SchillingV. HejnyMartin SchumacherH. J. ArendsM. Langsubject
PhysicsNuclear and High Energy PhysicsBackscatterProton010308 nuclear & particles physicsAstrophysics::High Energy Astrophysical PhenomenaNuclear TheoryCompton scattering01 natural sciencesNuclear physicsDeuteriumPolarizabilityDispersion relation0103 physical sciencesNeutronAtomic physicsNuclear Experiment010306 general physicsSpin-½description
Differential cross sections for Compton scattering from the free proton at Theta(gamma)(lab) = 130.7 degrees in the energy region from 200 MeV to 410 MeV and far quasi-free Compton scattering from the proton bound in the deuteron at Theta(gamma)(lab) = 148.8 degrees in the energy region from 200 MeV to 290 MeV have been measured. The free proton data are in agreement with dispersion-theory predictions based on standard parameters. The difference of the proton polarizabilities has been extracted from the quasi-free data. Our result, - = [9.1 +/- 1.7(stat + syst) +/- 1.2(mod)] x 10(-4) fm(3), is in reasonable agreement with the world average of the free proton data if the backward spin polarizability gamma(pi) is taken to be -37.6 x 10(-4) fm(4) as predicted by dispersion theory in agreement with many theoretical calculations. This implies that quasi-free Compton scattering may also be used to determine the electromagnetic polarizabilities of the neutron. No indication has been found of a recently suggested new contribution to gamma(pi).
year | journal | country | edition | language |
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1999-11-01 |