Strong decays of $a_0$, $f_0$, $f_2$, and $K^*_2$ resonances as dynamically generated states of two vector mesons

Qing-Hua Shen, Li-Sheng Geng, Ju-Jun Xie
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引用次数: 0

Abstract

The two-body strong decays of the $f_0(1500)$, $f_0(1710)$, $a_0(1710)$, $f_2(1270)$, $f_2'(1525)$, and $K_2^*(1430)$ resonances are investigated, assuming them as dynamically generated states of two vector mesons via $s$-wave interactions. The partial decay widths of all the possible two-body pseudoscalar meson-pseudoscalar meson final states are calculated considering the triangular diagrams. It is found that the ratios of branching fractions are similar to the previous results for most channels, which were obtained by using the real-axis method and considering the box diagrams. However, there are also differences. In addition, our focus is on the partial decay widths. More precise experimental measurements are needed to test the model calculations and determine the nature of these scalar and tensor mesons. It is anticipated that the BES\uppercase\expandafter{\romannumeral3}, Belle\uppercase\expandafter{\romannumeral2} and LHCb collaborations will conduct these measurements in the future.
作为两个矢量介子动态生成态的 $a_0$、$f_0$、$f_2$ 和 $K^*_2$ 共振的强衰变
研究了$f_0(1500)$、$f_0(1710)$、$a_0(1710)$、$f_2(1270)$、$f_2'(1525)$和$K_2^*(1430)$共振的二体强衰变,假定它们是两个矢量介子通过$s$波相互作用动态生成的态。考虑到三角形图,计算了所有可能的二体伪介子-伪介子终态的部分衰变宽度。结果发现,对于大多数信道来说,分支分数的比值与以前通过使用实轴方法和考虑方框图得到的结果相似。然而,两者也存在差异。此外,我们的重点是部分衰变宽度。我们需要更精确的实验测量来检验模型计算,并确定这些标量和张量介子的性质。预计BESuppercase/expandafter{romannumeral3}、Belleuppercase/expandafter{romannumeral2}和LHCb合作组将在未来进行这些测量。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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