标量 $f_0(500)$ 和 $f_0(980)$ 在 $D^0\to π^0π^0 \bar{K}^0$ 过程中的作用

Xiao-Hui Zhang, Han Zhang, Bai-Cian Ke, Li-Juan Liu, De-Min Li, En Wang
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引用次数: 0

摘要

我们在研究这个过程时,考虑到了手性单位方法中$S$波伪正射介子-伪正射介子相互作用的贡献,以及中间共振$K^{*}(892)$的贡献。我们的结果与CLEO测量结果非常吻合,这意味着在$\pi^0\pi^0$阈值附近的近阈值增强主要是由于标量介子$f_0(500)$和中间的$K^*$的贡献,而$\pi^0\pi^0$不变质量分布中1~GeV附近的尖顶结构应该与标量介子$f_0(980)$有关。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Roles of the scalar $f_0(500)$ and $f_0(980)$ in the process $D^0\to π^0π^0 \bar{K}^0$
Motivated by the near-threshold enhancement and the dip structure around 1~GeV in the $\pi^0\pi^0$ invariant mass distribution of the process $D^0\to \pi^0\pi^0\bar{K}^0$ observed by the CLEO Collaboration, we have investigated this process by taking into account the contribution from the $S$-wave pseudoscalar meson-pseudoscalar meson interactions within the chiral unitary approach, and also the one from the intermediate resonance $K^{*}(892)$. Our results are in good agreement with the CLEO measurements, which implies that, the near-threshold enhancement near the $\pi^0\pi^0$ threshold is mainly due to the contributions from the scalar meson $f_0(500)$ and the intermediate $K^*$, and the cusp structure around 1~GeV in the $\pi^0\pi^0$ invariant mass distribution should be associated with the scalar meson $f_0(980)$.
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