Measurement of the helicity asymmetry E in ω→π^+π^-π^0 photoproduction

Z. Akbar,P. Roy,S. Park,V. Crede,A. V. Anisovich,I. Denisenko,E. Klempt,V. A. Nikonov,A. V. Sarantsev,K. P. Adhikari,S. Adhikari,M. J. Amaryan,S. Anefalos Pereira,H. Avakian,J. Ball,M. Battaglieri,V. Batourine,I. Bedlinskiy,S. Boiarinov,W. J. Briscoe,J. Brock,W. K. Brooks,V. D. Burkert, F. T. Cao,C. Carlin,D. S. Carman,A. Celentano,G. Charles,T. Chetry,G. Ciullo,L. Clark,P. L. Cole,M. Contalbrigo,O. Cortes,A. D'Angelo,N. Dashyan,R. De Vita,E. De Sanctis, A. Deur,C. Djalali,M. Dugger,R. Dupre,H. Egiyan,L. El Fassi,P. Eugenio,G. Fedotov,R. Fersch,A. Filippi,A. Fradi,M. Garcon, N. Gevorgyan, K. L. Giovanetti,F. X. Girod,C. Gleason,W. Gohn,E. Golovach, R. W. Gothe, K. A. Griffioen,M. Guidal,L. Guo,K. Hafidi,H. Hakobyan,C. Hanretty,N. Harrison,M. Hattawy,D. Heddle,K. Hicks,G. Hollis,M. Holtrop,D. G. Ireland,B. S. Ishkhanov,E. L. Isupov,D. Jenkins,S. Joosten,C. D. Keith,D. Keller,G. Khachatryan,M. Khachatryan,M. Khandaker,A. Kim,W. Kim,A. Klein,F. J. Klein,V. Kubarovsky,L. Lanza,K. Livingston,I. J. D. MacGregor,N. Markov,B. McKinnon,D. G. Meekins,T. Mineeva,V. Mokeev,A. Movsisyan,C. Munoz Camacho,P. Nadel-Turonski,S. Niccolai,M. Osipenko, A. I. Ostrovidov,M. Paolone,R. Paremuzyan,K. Park,E. Pasyuk,W. Phelps,O. Pogorelko,J. W. Price,Y. Prok,D. Protopopescu,B. A. Raue, M. Ripani,B. G. Ritchie,A. Rizzo,G. Rosner,F. Sabatie,C. Salgado,R. A. Schumacher,Y. G. Sharabian,Iu. Skorodumina,G. D. Smith,D. I. Sober,D. Sokhan,N. Sparveris,S. Stepanyan,I. I. Strakovsky,S. Strauch,M. Taiuti,M. Ungaro,H. Voskanyan,E. Voutier,X. Wei,M. H. Wood,N. Zachariou,L. Zana,J. Zhang,Z. W. Zhao

PHYSICAL REVIEW C(2017)

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摘要
The double-polarization observable E was studied for the reaction γ p→ pω using the CEBAF Large Acceptance Spectrometer (CLAS) in Hall B at the Thomas Jefferson National Accelerator Facility and the longitudinally-polarized frozen-spin target (FROST). The observable was measured from the charged decay mode of the meson, ω→π^+π^-π^0, using a circularly-polarized tagged-photon beam with energies ranging from the ω threshold at 1.1 to 2.3 GeV. A partial-wave analysis within the Bonn-Gatchina framework found dominant contributions from the 3/2^+ partial wave near threshold, which is identified with the sub-threshold N(1720) 3/2^+ nucleon resonance. To describe the entire data set, which consisted of ω differential cross sections and a large variety of polarization observables, further contributions from other nucleon resonances were found to be necessary. With respect to non-resonant mechanisms, π exchange in the t-channel was found to remain small across the analyzed energy range, while pomeron t-channel exchange gradually grew from the reaction threshold to dominate all other contributions above W ≈ 2 GeV.
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