Photoproduction of the $f_1(1285)$ Meson

R. Dickson,J. W. Price,E. Munevar,M. J. Amaryan,G. Fedotov,V. Batourine,W. J. Briscoe,S. Anefalos Pereira,S. Chandavar,E. De Sanctis,P. Nadel-Turonski,G. P. Gilfoyle,S. Stepanyan,H. Y. Lu, H. Hakobyan,G. Charles,A. Deur,L. Lanza,Z. Akbar, P. Mattione,M. Battaglieri,A. Kim,S. Joosten,T. Cao,D. S. Carman,A. Ni, N. Gevorgyan,M. Hattawy,I. Bedlinskiy,G. Ciullo,A. Rizzo,V. Kubarovsky, E. Seder,P. Eugenio,L. Guo,E. Fanchini,F. X. Girod,H. Voskanyan,E. Pasyuk,M. H. Wood,G. D. Smith,Y. Ilieva, D. Sokhan,B. A. Raue, R. Badui, D. I. Sober,N. Markov,C. Djalali,M. Holtrop,M. Dugger,W. Phelps,A. S. Biselli,M. Mirazita,K. A. Griffioen,V. Mokeev,I. Stankovic,T. Chetry,N. Zachariou,K. Hicks,B. S. Ishkhanov,N. Harrison,D. Keller,M. Contalbrigo,O. Cortes, G. Rosner,B. McKinnon, I. J. D. MacGregor,H. S. Jo,R. De Vita, K. Park, K. Livingston,R. W. Gothe,L. Colaneri, L. A. Net,N. Dashyan,F. Klein,K. Hafidi,G. Murdoch,S. Boiarinov,V. Sytnik,W. Kim,K. P. Adhikari,S. V. Kuleshov, M. Ungaro, I. Zonta,V. D. Burkert,N. K. Walford,C. Meyer,L. El Fassi,R. A. Schumacher,N. Compton,K. Moriya,Y. Prok,S. M. Hughes,M. Taiuti,P. Roy,H. Jiang, C. Salgado,D. P. Watts,S. Strauch,A. D'Angelo,E. Voutier,S. Pisano, D. P. Weygand,J. Ball, E. S. Smith, M. Khandaker,A. I. Ostrovidov, P. Lenisa,J. A. Fleming,O. Pogorelko,J. Zhang,C. Hanretty,P. L. Cole,G. Khachatryan,A. Filippi,D. G. Ireland,R. Dupre,Y. Ghandilyan,N. Sparveris,A. Celentano,E. L. Isupov, L. Zana,K. L. Giovanetti,I. I. Strakovsky,A. El Alaoui,Y. G. Sharabian,M. Osipenko,Iu. Skorodumina, M. Ripani,A. J. R. Puckett

Bulletin of the American Physical Society(2016)

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摘要
The f(1)(1285) meson withmass 1281.0 +/- 0.8MeV/c(2) and width 18.4 +/- 1.4MeV (full width at half maximum) was measured for the first time in photoproduction from a proton target using CLAS at Jefferson Lab. Differential cross sections were obtained via the eta pi(+)pi(-), K+(K) over bar (0) pi(-), and (K-K0)pi(+) decay channels from threshold up to a center-of-mass energy of 2.8 GeV. The mass, width, and an amplitude analysis of the eta pi(+)pi(-) final-state Dalitz distribution are consistent with the axial-vector J(P) = 1(+) f(1)(1285) identity, rather than the pseudoscalar 0(-) eta(1295). The production mechanism is more consistent with s-channel decay of a high-mass N* state and not with t-channel meson exchange. Decays to eta pi pi go dominantly via the intermediate a(0)(+/-) (980)pi(-/+) states, with the branching ratio Gamma [a(0)pi (no (K) over barK)]/Gamma[eta pi pi (all)] = 0.74 +/- 0.09. The branching ratios Gamma (K (K) over bar pi)/Gamma(eta pi pi) = 0.216 +/- 0.033 and Gamma (gamma rho(0))/Gamma(eta pi pi) = 0.047 +/- 0.018 were also obtained. The first is in agreement with previous data for the f(1)(1285), while the latter is lower than the world average.
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