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Differential Cross Section and Photon-Beam Asymmetry for the gamma(->)p -> Pi(-)Delta(+ +) (1232) Reaction at Forward Pi(-) Angles for E-gamma=1.5-2.95 GeV

Authors
Kohri, H.Shiu, S. H.Chang, W. C.Yanai, Y.Ahn, D. S.Ahn, J. K.Chen, J. Y.Date, S.Ejiri, H.Fujimura, H.Fujiwara, M.Fukui, S.Gohn, W.Hicks, K.Hosaka, A.Hotta, T.Hwang, S. H.Imai, K.Ishikawa, T.Joo, K.Kato, Y.Kon, Y.Lee, H. S.Maeda, Y.Mibe, T.Miyabe, M.Morino, Y.Muramatsu, N.Nakano, T.Nakatsugawa, Y.Nam, S., INiiyama, M.Noumi, H.Ohashi, Y.Ohta, T.Oka, M.Parker, J. D.Rangacharyulu, C.Ryu, S. Y.Sawada, T.Shimizu, H.Strokovsky, E. A.Sugaya, Y.Sumihama, M.Tsunemi, T.Uchida, M.Ungaro, M.Wang, S. Y.Yosoi, M.
Issue Date
18-May-2018
Publisher
AMER PHYSICAL SOC
Citation
PHYSICAL REVIEW LETTERS, v.120, no.20
Indexed
SCIE
SCOPUS
Journal Title
PHYSICAL REVIEW LETTERS
Volume
120
Number
20
URI
https://scholar.korea.ac.kr/handle/2021.sw.korea/75511
DOI
10.1103/PhysRevLett.120.202004
ISSN
0031-9007
Abstract
Differential cross sections and photon-beam asymmetries for the gamma(->)p -> Pi(-)Delta(++)(1232) reaction have been measured for 0.7 < cos Theta(c.m.)(Pi) < 1 and E-gamma= 1.5-2.95 GeV at SPring-8/LEPS. The first-ever high statistics cross-section data are obtained in this kinematical region, and the asymmetry data for 1.5 < E-gamma(GeV) < 2.8 are obtained for the first time. This reaction has a unique feature for studying the production mechanisms of a pure uu quark pair in the final state from the proton. Although there is no distinct peak structure in the cross sections, a non-negligible excess over the theoretical predictions is observed at E-gamma= 1.5-1.8 GeV. The asymmetries are found to be negative in most of the present kinematical regions, suggesting the dominance of n exchange in the t channel. The negative asymmetries at forward meson production angles are different from the asymmetries previously measured for the photoproduction reactions producing a dd(-) or an ss quark pair in the final state. Advanced theoretical models introducing nucleon resonances and additional unnatural-parity exchanges are needed to reproduce the present data.
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