Xiao-Hui Zhang, Han Zhang, Bai-Cian Ke, Li-Juan Liu, De-Min Li, En Wang
{"title":"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","authors":"Xiao-Hui Zhang, Han Zhang, Bai-Cian Ke, Li-Juan Liu, De-Min Li, En Wang","doi":"arxiv-2409.09966","DOIUrl":null,"url":null,"abstract":"Motivated by the near-threshold enhancement and the dip structure around\n1~GeV in the $\\pi^0\\pi^0$ invariant mass distribution of the process $D^0\\to\n\\pi^0\\pi^0\\bar{K}^0$ observed by the CLEO Collaboration, we have investigated\nthis process by taking into account the contribution from the $S$-wave\npseudoscalar meson-pseudoscalar meson interactions within the chiral unitary\napproach, and also the one from the intermediate resonance $K^{*}(892)$. Our\nresults are in good agreement with the CLEO measurements, which implies that,\nthe near-threshold enhancement near the $\\pi^0\\pi^0$ threshold is mainly due to\nthe contributions from the scalar meson $f_0(500)$ and the intermediate $K^*$,\nand the cusp structure around 1~GeV in the $\\pi^0\\pi^0$ invariant mass\ndistribution should be associated with the scalar meson $f_0(980)$.","PeriodicalId":501067,"journal":{"name":"arXiv - PHYS - High Energy Physics - Phenomenology","volume":"15 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Roles of the scalar $f_0(500)$ and $f_0(980)$ in the process $D^0\\\\to π^0π^0 \\\\bar{K}^0$\",\"authors\":\"Xiao-Hui Zhang, Han Zhang, Bai-Cian Ke, Li-Juan Liu, De-Min Li, En Wang\",\"doi\":\"arxiv-2409.09966\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"Motivated by the near-threshold enhancement and the dip structure around\\n1~GeV in the $\\\\pi^0\\\\pi^0$ invariant mass distribution of the process $D^0\\\\to\\n\\\\pi^0\\\\pi^0\\\\bar{K}^0$ observed by the CLEO Collaboration, we have investigated\\nthis process by taking into account the contribution from the $S$-wave\\npseudoscalar meson-pseudoscalar meson interactions within the chiral unitary\\napproach, and also the one from the intermediate resonance $K^{*}(892)$. Our\\nresults are in good agreement with the CLEO measurements, which implies that,\\nthe near-threshold enhancement near the $\\\\pi^0\\\\pi^0$ threshold is mainly due to\\nthe contributions from the scalar meson $f_0(500)$ and the intermediate $K^*$,\\nand the cusp structure around 1~GeV in the $\\\\pi^0\\\\pi^0$ invariant mass\\ndistribution should be associated with the scalar meson $f_0(980)$.\",\"PeriodicalId\":501067,\"journal\":{\"name\":\"arXiv - PHYS - High Energy Physics - Phenomenology\",\"volume\":\"15 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2024-09-16\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv - PHYS - High Energy Physics - Phenomenology\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/arxiv-2409.09966\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - PHYS - High Energy Physics - Phenomenology","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.09966","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
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 $f_0(980)$.