Analysis of the data for γp → f1(1285)p photoproduction

Ai-Chao Wang, N. Wei, Fei Huang
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Abstract

The photoproduction of f1(1285) meson off proton is investigated within an effective Lagrangian approach. The t-channel ρ- and ω-exchange diagrams, u-channel nucleon-exchange diagram, generalized contact term, and s-channel pole diagrams of nucleon and a minimal number of nucleon resonances are taken into account in constructing the reaction amplitudes to describe the experimental data. Three different models, i.e., the Feynman model, the Regge model, and the interpolated Regge model, are employed where the t-channel reaction amplitudes are constructed in Feynman type, Regge type, and interpolated Regge type, respectively. The results show that in neither Feynman model nor interpolated Regge model can the available data for γp → f1(1285)p be satisfactorily reproduced. Nevertheless, in the Regge model, when any one of the N(1990)7/2+, N(2000)5/2+, N(2040)3/2+, N(2060)5/2−, N(2100)1/2+, N(2120)3/2−, N(2190)7/2−, N(2300)1/2+, and N(2570)5/2−resonances is considered, the data can be well described. The resulted resonance parameters are consistent with those advocated in Particle Data Group (PDG) review. Further analysis shows that in high-energy region, the peaks of γp → f1(1285)p differential cross sections at forward angles are dominated by the contributions from t-channel ρ- and ω-exchange diagrams, while in low-energy region, the s-channel pole diagrams of resonances also provide significant contributions to the γp → f1(1285)p cross sections.
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γp→f1(1285)p光生成数据分析
在有效拉格朗日方法中研究了质子外f1(1285)介子的光生成。在构建描述实验数据的反应振幅时,考虑了核子的 t 道 ρ- 和 ω 交换图、u 道核子交换图、广义接触项和 s 道极点图以及极少数量的核子共振。采用了三种不同的模型,即费曼模型、雷格模型和插值雷格模型,分别以费曼型、雷格型和插值雷格型构建 t 道反应振幅。结果表明,在费曼模型和插值雷格模型中,γp → f1(1285)p 的现有数据都不能令人满意地再现。然而,在雷格模型中,当考虑 N(1990)7/2+、N(2000)5/2+、N(2040)3/2+、N(2060)5/2-、N(2100)1/2+、N(2120)3/2-、N(2190)7/2-、N(2300)1/2+ 和 N(2570)5/2 共振中的任何一个共振时,数据都能得到很好的描述。得出的共振参数与粒子数据小组(PDG)评论中主张的参数一致。进一步的分析表明,在高能区,γp → f1(1285)p差分截面在正向角的峰值主要来自t沟道ρ-和ω-交换图的贡献,而在低能区,共振的s沟道极图也对γp → f1(1285)p截面有重要贡献。
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