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dc.creatorGolovatch, E
dc.creatorBurkert, VD
dc.creatorCarman, DS
dc.creatorGothe, RW
dc.creatorHicks, K
dc.creatorIshkhanov, BS
dc.creatorMokeev, VI
dc.creatorPasyuk, E
dc.creatorAdhikari, S
dc.creatorAkbar, Z
dc.creatorAmaryan, MJ
dc.creatorAvakian, H
dc.creatorBall, J
dc.creatorBarion, L
dc.creatorBashkanov, M
dc.creatorBattaglieri, M
dc.creatorBedlinskiy, I
dc.creatorBiselli, AS
dc.creatorBoiarinov, S
dc.creatorBriscoe, WJ
dc.creatorCao, F
dc.creatorCelentano, A
dc.creatorChatagnon, P
dc.creatorChetry, T
dc.creatorCiullo, G
dc.creatorClark, L
dc.creatorClary, BA
dc.creatorCole, PL
dc.creatorContalbrigo, M
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.creatorDiehl, S
dc.creatorDjalali, C
dc.creatorDugger, M
dc.creatorDupre, R
dc.creatorEgiyan, H
dc.creatorEhrhart, M
dc.creatorEl Alaoui, A
dc.creatorEl Fassi, L
dc.creatorElouadrhiri, L
dc.creatorEugenio, P
dc.creatorFedotov, G
dc.creatorFersch, R
dc.creatorFilippi, A
dc.creatorGhandilyan, Y
dc.creatorGilfoyle, GP
dc.creatorGiovanetti, KL
dc.creatorGirod, FX
dc.creatorGlazier, DI
dc.creatorGriffioen, KA
dc.creatorGuidal, M
dc.creatorGuo, L
dc.creatorHafidi, K
dc.creatorHakobyan, H
dc.creatorHarrison, N
dc.creatorHattawy, M
dc.creatorHeddle, D
dc.creatorHoltrop, M
dc.creatorIlieva, Y
dc.creatorIreland, DG
dc.creatorIsupov, EL
dc.creatorJenkins, D
dc.creatorJo, HS
dc.creatorJohnston, S
dc.creatorJoo, K
dc.creatorKabir, ML
dc.creatorKeller, D
dc.creatorKhachatryan, G
dc.creatorKhachatryan, M
dc.creatorKhandaker, M
dc.creatorKim, W
dc.creatorKlein, A
dc.creatorKlein, FJ
dc.creatorKubarovsky, V
dc.creatorLanza, L
dc.creatorLenisa, P
dc.creatorLivingston, K
dc.creatorMacGregor, IJD
dc.creatorMarchand, D
dc.creatorMarkov, N
dc.creatorMcKinnon, B
dc.creatorMeyer, CA
dc.creatorMontgomery, RA
dc.creatorMovsisyan, A
dc.creatorMunoz Camacho, C
dc.creatorNadel-Turonski, P
dc.creatorNiccolai, S
dc.creatorNiculescu, G
dc.creatorOsipenko, M
dc.creatorOstrovidov, AI
dc.creatorPaolone, M
dc.creatorParemuzyan, R
dc.creatorPark, K
dc.creatorPogorelko, O
dc.creatorPrice, JW
dc.date.accessioned2020-12-11T20:18:28Z
dc.date.available2020-12-11T20:18:28Z
dc.date.issued2019-01-10
dc.identifier.issn0370-2693
dc.identifier.issn1873-2445
dc.identifier.doihttp://dx.doi.org/10.34944/dspace/4333
dc.identifier.otherHG9XD (isidoc)
dc.identifier.urihttp://hdl.handle.net/20.500.12613/4351
dc.description.abstract© 2018 The Author We report the first experimental measurements of the nine 1-fold differential cross sections for the γp→π+π−p reaction, obtained with the CLAS detector at Jefferson Laboratory. The measurements cover the invariant mass range of the final state hadrons from 1.6 GeV <W< 2.0 GeV. For the first time the photocouplings of all prominent nucleon resonances in this mass range have been extracted from this exclusive channel. Photoproduction of two charged pions is of particular importance for the evaluation of the photocouplings for the Δ(1620)1/2−, Δ(1700)3/2−, N(1720)3/2+, and Δ(1905)5/2+ resonances, which have dominant decays into the ππN final states rather than the more extensively studied single meson decay channels.
dc.format.extent371-379
dc.language.isoen
dc.relation.haspartPhysics Letters, Section B: Nuclear, Elementary Particle and High-Energy Physics
dc.relation.isreferencedbyElsevier BV
dc.rights.urihttps://creativecommons.org/licenses/by/4.0/
dc.subjectTwo pion photoproduction
dc.subjectResonance photocouplings
dc.subjectBaryon state
dc.titleFirst results on nucleon resonance photocouplings from the γp → π+π−p reaction
dc.typeArticle
dc.type.genreJournal Article
dc.relation.doi10.1016/j.physletb.2018.10.013
dc.ada.noteFor Americans with Disabilities Act (ADA) accommodation, including help with reading this content, please contact scholarshare@temple.edu
dc.date.updated2020-12-11T20:18:24Z
refterms.dateFOA2020-12-11T20:18:29Z


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