First measurement of direct photoproduction of the a2(1320)0 meson on the proton
A. Celentano,M. Battaglieri,R. De Vita,L. Marsicano,V. Mathieu,A. Pilloni,A.P. Szczepaniak,K. P. Adhikari,S. Adhikari,M. J. Amaryan,G. Angelini,H. Atac,L. Barion,I. Bedlinskiy,F. Benmokhtar,A. Bianconi,A. S. Biselli,F. Bossú,S. Boiarinov,W. J. Briscoe,W. K. Brooks,D. Bulumulla,V. D. Burkert,D. S. Carman,J. Carvajal,P. Chatagnon,T. Chetry,G. Ciullo,L. Clark,P. L. Cole,M. Contalbrigo,O. Cortes,V. Credé,R. Cruz-Torres,A. D’Angelo,N. Dashyan,M. Defurne,A. Deur,Stefan Diehl,C. Djalali,M. Dugger,R. Dupré,H. Egiyan,M. Ehrhart,A. El Alaoui,L. El Fassi,L. Elouadrhiri,P. Eugenio,G. Fedotov,R. Fersch,A. Filippi,G. Gavalian,N. Gevorgyan,F. X. Girod,D. I. Glazier,W. Gohn,E. Golovatch,R. Gothe,K. A. Griffioen,M. Guidal,K. Hafidi,H. Hakobyan,N. Harrison,M. Hattawy,F. Hauenstein,T. B. Hayward,D. Heddle,K. Hicks,A. Hobart,M. Holtrop,Y. Ilieva,D. G. Ireland,B. S. Ishkhanov,E. L. Isupov,D. Jenkins,H. S. Jo,K. Joo,S. Joosten,D. Keller,M. Khachatryan,A. Khanal,M. Khandaker,A. Kim,C. W. Kim,W. Kim,F. J. Klein,V. Kubarovsky,L. Lanza,M. Leali,P. Lenisa,K. Livingston,V. Lucherini,I. J. D. MacGregor,D. Marchand,N. Markov,V. Mascagna,M. E. McCracken,B. McKinnon,Zein‐Eddine Meziani,M. Mirazita,V. Mokeev,A. Movsisyan,E. Munévar,C. Muñoz Camacho,P. Nadel-Turoński,K. Neupane,S. Niccolai,G. Niculescu,M. Osipenko,A. I. Ostrovidov,M. Paolone,L. L. Pappalardo,R. Paremuzyan,E. Pasyuk,W. Phelps,O. Pogorelko,J. W. Price,Y. Prok,M. Ripani,J. Ritman,A. Rizzo,G. Rosner,J. Rowley,F. Sabatié,C. Salgado,Axel Schmidt,R. A. Schumacher,Uttam Shrestha,D. Sokan,O. Soto,N. Sparveris,S. Stepanyan,I. I. Strakovsky,S. Strauch,J. A. Tan,N. J. C. Tyler,M. Ungaro,L. Venturelli,H. Voskanyan,E. Voutier,D. P. Watts,Xin Wei,M. H. Wood,N. Zachariou,J. Zhang,Z. W. Zhao
Physical Review C(2020)
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摘要
We present the first measurement of the reaction $\ensuremath{\gamma}p\ensuremath{\rightarrow}{a}_{2}{(1320)}^{0}\phantom{\rule{0.16em}{0ex}}p$ in the photon energy range 3.5--$5.5\phantom{\rule{0.16em}{0ex}}\mathrm{Ge}\mathrm{V}$ and four-momentum transfer squared $0.2<\ensuremath{-}t<2.0{\phantom{\rule{0.16em}{0ex}}\mathrm{Ge}\mathrm{V}}^{2}$. Data were collected with the CEBAF Large Acceptance Spectrometer detector at the Thomas Jefferson National Accelerator Facility. The ${a}_{2}$ resonance was detected by measuring the reaction $\ensuremath{\gamma}p\ensuremath{\rightarrow}{\ensuremath{\pi}}^{0}\ensuremath{\eta}p$ and reconstructing the ${\ensuremath{\pi}}^{0}\ensuremath{\eta}$ invariant mass. The most prominent feature of the differential cross section is a dip at $\ensuremath{-}t\ensuremath{\approx}0.55{\phantom{\rule{0.16em}{0ex}}\mathrm{Ge}\mathrm{V}}^{2}$. This can be described in the framework of Regge phenomenology, where the exchange degeneracy hypothesis predicts a zero in the reaction amplitude for this value of the four-momentum transfer.