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dc.creatorMattione, PT
dc.creatorCarman, DS
dc.creatorStrakovsky, II
dc.creatorWorkman, RL
dc.creatorKudryavtsev, AE
dc.creatorSvarc, A
dc.creatorTarasov, VE
dc.creatorAdhikari, KP
dc.creatorAdhikari, S
dc.creatorAdikaram, D
dc.creatorAkbar, Z
dc.creatorAnefalos Pereira, S
dc.creatorBall, J
dc.creatorBaltzell, NA
dc.creatorBashkanov, M
dc.creatorBattaglieri, M
dc.creatorBatourine, V
dc.creatorBedlinskiy, I
dc.creatorBiselli, AS
dc.creatorBoiarinov, S
dc.creatorBriscoe, WJ
dc.creatorBurkert, VD
dc.creatorCao, T
dc.creatorCelentano, A
dc.creatorCharles, G
dc.creatorChetry, T
dc.creatorCiullo, G
dc.creatorClark, L
dc.creatorCole, PL
dc.creatorContalbrigo, M
dc.creatorCortes, O
dc.creatorCrede, V
dc.creatorD'Angelo, A
dc.creatorDashyan, N
dc.creatorDe Vita, R
dc.creatorDe Sanctis, E
dc.creatorDefurne, M
dc.creatorDeur, A
dc.creatorDjalali, C
dc.creatorDugger, M
dc.creatorDupre, R
dc.creatorEgiyan, H
dc.creatorEl Alaoui, A
dc.creatorEl Fassi, L
dc.creatorEugenio, P
dc.creatorFedotov, G
dc.creatorFersch, R
dc.creatorFilippi, A
dc.creatorFleming, JA
dc.creatorFradi, A
dc.creatorGhandilyan, Y
dc.creatorGilfoyle, GP
dc.creatorGiovanetti, KL
dc.creatorGirod, FX
dc.creatorGleason, C
dc.creatorGolovatch, E
dc.creatorGothe, RW
dc.creatorGriffioen, KA
dc.creatorGuidal, M
dc.creatorHafidi, K
dc.creatorHakobyan, H
dc.creatorHanretty, C
dc.creatorHarrison, N
dc.creatorHattawy, M
dc.creatorHeddle, D
dc.creatorHicks, K
dc.creatorHollis, G
dc.creatorHoltrop, M
dc.creatorHughes, SM
dc.creatorIlieva, Y
dc.creatorIreland, DG
dc.creatorIshkhanov, BS
dc.creatorIsupov, EL
dc.creatorJenkins, D
dc.creatorJiang, H
dc.creatorJo, HS
dc.creatorJoo, K
dc.creatorJoosten, S
dc.creatorKeller, D
dc.creatorKhachatryan, G
dc.creatorKhachatryan, M
dc.creatorKhandaker, M
dc.creatorKim, A
dc.creatorKim, W
dc.creatorKlein, A
dc.creatorKlein, FJ
dc.creatorKubarovsky, V
dc.creatorKuleshov, SV
dc.creatorLanza, L
dc.creatorLenisa, P
dc.creatorLivingston, K
dc.creatorMacGregor, IJD
dc.creatorMarkov, N
dc.creatorMcKinnon, B
dc.creatorMeyer, CA
dc.creatorMeziani, ZE
dc.creatorMineeva, T
dc.creatorMokeev, V
dc.creatorMontgomery, RA
dc.creatorMovsisyan, A
dc.date.accessioned2021-02-02T23:58:55Z
dc.date.available2021-02-02T23:58:55Z
dc.date.issued2017-09-18
dc.identifier.issn2469-9985
dc.identifier.issn2469-9993
dc.identifier.doihttp://dx.doi.org/10.34944/dspace/5658
dc.identifier.otherFH3WA (isidoc)
dc.identifier.urihttp://hdl.handle.net/20.500.12613/5676
dc.description.abstract© 2017 American Physical Society. The quasifree γd→π-p(p) differential cross section has been measured with CLAS at photon beam energies Eγ from 0.445 to 2.510 GeV (corresponding to W from 1.311 to 2.366 GeV) for pion center-of-mass angles cosθπc.m. from -0.72 to 0.92. A correction for final state interactions has been applied to these data to extract the γn→π-p differential cross sections. These cross sections are quoted in 8428 (Eγ,cosθπc.m.) bins, a factor of nearly 3 increase in the world statistics for this channel in this kinematic range. These new data help to constrain coupled-channel analysis fits used to disentangle the spectrum of N∗ resonances and extract their properties. Selected photon decay amplitudes N∗→γn at the resonance poles are determined for the first time and are reported here.
dc.format.extent035204-
dc.language.isoen
dc.relation.haspartPhysical Review C
dc.relation.isreferencedbyAmerican Physical Society (APS)
dc.subjectnucl-ex
dc.subjectnucl-ex
dc.titleDifferential cross section measurements for γn→π-p above the first nucleon resonance region
dc.typeArticle
dc.type.genreJournal Article
dc.relation.doi10.1103/PhysRevC.96.035204
dc.ada.noteFor Americans with Disabilities Act (ADA) accommodation, including help with reading this content, please contact scholarshare@temple.edu
dc.date.updated2021-02-02T23:58:50Z
refterms.dateFOA2021-02-02T23:58:55Z


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