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On the near-threshold peak structure in the differential cross section of \phi-meson photoproduction: indication of a missing resonance with non-negligible strangeness content

机译:在差分截面上的近阈值峰值结构   \ phi-meson photoproduction:表示缺失共振   不可忽视的陌生内容

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摘要

The details of the analysis of the near-threshold bump structure in theforward differential cross section of the \phi-meson photoproduction todetermine whether it is a signature of a resonance are presented. The analysisis carried out in an effective Lagrangian approach which includes Pomeron and(\pi,\eta) exchanges in the t channel, and contributions from the s- andu-channel excitations of a postulated nucleon resonance. In addition to thedifferential cross sections, we use the nine spin-density matrix elements(SDME) as recently measured, instead of the phi-meson decay angulardistributions which depend only on six SDMEs as was done before, to constrainthe resonance parameters. We conclude that indeed the nonmonotonic behavior,along with the other experimental data as reported by LEPS, can only beexplained with an assumption of the excitation of a resonance of spin 3/2, aspreviously reported. However, both parities can account for the data equallywell with almost identical mass of 2.08 +/- 0.04 GeV and width of 0.501 +/-0.117 and 0.570 +/- 0.159 for 3/2^+ and 3/2^-, respectively. The ratio of thehelicity amplitudes A_{1/2}/A_{3/2} calculated from the resulting couplingconstants differs in sign from that of the known D_{13}(2080). Moreexperimental data on single and double polarization observables are needed toresolve the parity. We further find that with an assumption of large values ofthe OZI-evading parameters x_{OZI} = 12 for J^P = 3/2^- and x_{OZI} = 9 for J^P= 3/2^+, the discrepancy between the recent experimental data on \omega-mesonphotoproduction and theoretical model can be considerably reduced. We arguethat the large value of x_{OZI} indicates that the postulated resonancecontains non-negligible amount of strangeness content.
机译:给出了在φ介子光子产生的前微分截面中分析近阈值凸起结构以确定其是否为共振信号的详细分析。该分析是在有效的拉格朗日方法中进行的,该方法包括t通道中的Pomeron和(\ pi,\ eta)交换,以及假定的核共振的s和u通道激发的贡献。除了微分截面外,我们还使用最近测量的九个自旋密度矩阵元素(SDME),而不是像以前那样仅依赖六个SDME的phi-介子衰变角分布来约束共振参数。我们得出的结论是,确实,非单调性行为以及LEPS报告的其他实验数据只能通过假设激发自旋3/2的共振来解释,如先前报道。然而,对于3/2 ^ +和3/2 ^-,两个奇偶校验都可以很好地解释数据,质量几乎相同,为2.08 +/- 0.04 GeV,宽度分别为0.501 +/- 0.117和0.570 +/- 0.159。由所得到的耦合常数计算出的螺旋度振幅的比率A_ {1/2} / A_ {3/2}的符号与已知的D_ {13}(2080)的符号不同。需要更多关于单极化和双极化可观察物的实验数据来解决奇偶校验。我们进一步发现,假设对于J ^ P = 3/2 ^-的OZI规避参数x_ {OZI} = 12的值较大,而对于J ^ P = 3/2 ^ +的x_ {OZI} = 9,则Ω介子光产生的最新实验数据与理论模型之间的差异可以大大减少。我们认为x_ {OZI}的较大值表明假定的共振包含不可忽略的数量的陌生内容。

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