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Coherent photon scattering on nuclei in the Δ(1232) resonance region

dc.contributor.advisorCaplan, Henryen_US
dc.contributor.committeeMemberFriar, Jimen_US
dc.contributor.committeeMemberAsai, Juhachien_US
dc.contributor.committeeMemberTomusiak, Eden_US
dc.contributor.committeeMemberWissman, Franken_US
dc.contributor.committeeMemberArends, J.en_US
dc.contributor.committeeMemberBergstrom, Jacken_US
dc.contributor.committeeMemberMiller, Jimen_US
dc.contributor.committeeMemberNathan, Alen_US
dc.contributor.committeeMemberHayward, Evansen_US
dc.creatorIgarashi, Ryuichien_US
dc.date.accessioned2012-07-26T10:01:13Zen_US
dc.date.accessioned2013-01-04T04:48:06Z
dc.date.available2013-07-26T08:00:00Zen_US
dc.date.available2013-01-04T04:48:06Z
dc.date.created1993en_US
dc.date.issued1993en_US
dc.date.submitted1993en_US
dc.description.abstractAngular distributions for photon scattering from ¹²C have been measured at the Saskatchewan Accelerator Laboratory (SAL) high duty factor bremsstrahlung facility. Data were taken at 160, 200, 250 and 290 MeV endpoint energies and at angles ranging from 20 degrees to 150 degrees with the 53 cm diameter x 56 cm long Boston University Sodium Iodide (BUNI) detector. Coherently scattered photons were easily distinguished from neutral pion decay photons in detected energy spectra. The excellent resolution of the detector and the high duty cycle at SAL have made it possible to obtain new data on the angular distributions for elastic and, in some cases, for inelastic scattering as well. It was essential to distinguish between elastic scattering and inelastic scattering to the 4.44 MeV state in ¹²C. This was further complicated by the continuous nature of bremsstrahlung such that only a region within about 4 MeV of the endpoint could be used. Hence, precise energy calibration and stability of the calibration were required. Since elastic cross sections can be small, pileup transferring inelastic events into the elastic region was a concern and required careful attention. The angular distributions for elastic scattering were compared with a simple calculation of a dipole distribution weighted by the charge form factor and scaled by forward cross sections derived from total absorption cross sections with dispersion relations. This calculation badly underestimates cross sections at back angles. The more serious calculation with the Δ-hole model at 200 MeV overestimates the measurements at all angles. Some cross sections for inelastic scattering leading to the 4.44 MeV first excited state in carbon have been extracted. These cross sections are small compared to the elastic channel at forward angles, but are dominant at backward angles. Since this experiment was the first to separate elastic from inelastic photon scattering at these energies, these new data should stimulate further theoretical study.en_US
dc.identifier.urihttp://hdl.handle.net/10388/etd-07262012-100113en_US
dc.language.isoen_USen_US
dc.titleCoherent photon scattering on nuclei in the Δ(1232) resonance regionen_US
dc.type.genreThesisen_US
dc.type.materialtexten_US
thesis.degree.departmentPhysicsen_US
thesis.degree.disciplinePhysicsen_US
thesis.degree.grantorUniversity of Saskatchewanen_US
thesis.degree.levelDoctoralen_US
thesis.degree.nameDoctor of Philosophy (Ph.D.)en_US

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