{
  "_oai": {
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  "authors": [
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "Faculty of Mathematics and Physics, Huaiyin Institute of Technology, China"
        }
      ], 
      "surname": "Zhang", 
      "email": "zylyw@hyit.edu.cn", 
      "full_name": "Zhang,Ya-Lan", 
      "given_names": "Ya-Lan"
    }, 
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "Faculty of Mathematics and Physics, Huaiyin Institute of Technology, China"
        }
      ], 
      "surname": "Wang", 
      "email": "chaowang@nankai.edu.cn", 
      "full_name": "Wang,Chao", 
      "given_names": "Chao"
    }, 
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "Faculty of Mathematics and Physics, Huaiyin Institute of Technology, China"
        }
      ], 
      "surname": "Lin", 
      "email": "linyihit@hyit.edu.cn", 
      "full_name": "Lin,Yi", 
      "given_names": "Yi"
    }, 
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "Department of Physics and Institute of Theoretical Physics, Nanjing Normal University, China"
        }, 
        {
          "country": "China", 
          "value": "Jiangsu Key Laboratory for Numerical Simulation of Large Scale Complex Systems, Nanjing Normal University, China"
        }
      ], 
      "surname": "Xiao", 
      "email": "xiaozhenjun@njnu.edu.cn", 
      "full_name": "Xiao,Zhen-Jun", 
      "given_names": "Zhen-Jun"
    }
  ], 
  "titles": [
    {
      "source": "IOP", 
      "title": "Resonance contributions from  In Charmless Three-body Hadronic Meson Decays  "
    }
  ], 
  "dois": [
    {
      "value": "10.1088/1674-1137/acbaea"
    }
  ], 
  "publication_info": [
    {
      "journal_title": "Chinese Physics C", 
      "material": "article", 
      "journal_volume": "47", 
      "artid": "043112", 
      "year": 2023, 
      "journal_issue": "4"
    }
  ], 
  "$schema": "http://repo.scoap3.org/schemas/hep.json", 
  "acquisition_source": {
    "date": "2023-06-06T03:30:59.739206", 
    "source": "IOP", 
    "method": "IOP", 
    "submission_number": "6ab8f560041a11ee8e62c23b20d38f61"
  }, 
  "page_nr": [
    7
  ], 
  "license": [
    {
      "url": "http://creativecommons.org/licenses/by/3.0/", 
      "license": "CC-BY-3.0"
    }
  ], 
  "copyright": [
    {
      "statement": "\u00a9 2023 Chinese Physical Society and the Institute of High Energy Physics of the Chinese Academy of Sciences and the Institute of Modern Physics of the Chinese Academy of Sciences and IOP Publishing Ltd", 
      "year": "2023"
    }
  ], 
  "control_number": "76246", 
  "record_creation_date": "2023-03-08T03:30:21.587268", 
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      "version_id": "b82f3027-c86e-421b-9007-e3a1acf5f8af", 
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      "size": 153725
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      "key": "10.1088/1674-1137/acbaea.pdf", 
      "size": 1965790
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  ], 
  "collections": [
    {
      "primary": "Chinese Physics C"
    }
  ], 
  "arxiv_eprints": [
    {
      "categories": [
        "hep-ph", 
        "hep-ex"
      ], 
      "value": "2302.04533"
    }
  ], 
  "abstracts": [
    {
      "source": "IOP", 
      "value": "Within the framework of perturbative QCD factorization, we investigate the nonfactorizable contributions to the factorization-forbidden quasi-two-body decays   $ B_{(s)}\\rightarrow h\\chi_{c0}\\rightarrow h\\pi^+\\pi^-(K^+K^-) $   with   $ B_{(s)}\\rightarrow h\\chi_{c0}\\rightarrow h\\pi^+\\pi^-(K^+K^-) $  . We compare our predicted branching ratios for the   $ B_{(s)}\\rightarrow h\\chi_{c0}\\rightarrow h\\pi^+\\pi^-(K^+K^-) $   decay with available experiment data as well as predictions by other theoretical studies. The branching ratios of these decays are consistent with data and other theoretical predictions. However, in the Cabibbo-suppressed decays   $ B_{(s)}\\rightarrow h\\chi_{c0}\\rightarrow h\\pi^+\\pi^-(K^+K^-) $   with   $ B_{(s)}\\rightarrow h\\chi_{c0}\\rightarrow h\\pi^+\\pi^-(K^+K^-) $  , the values of the branching ratios are of the order of   $ B_{(s)}\\rightarrow h\\chi_{c0}\\rightarrow h\\pi^+\\pi^-(K^+K^-) $   and   $ B_{(s)}\\rightarrow h\\chi_{c0}\\rightarrow h\\pi^+\\pi^-(K^+K^-) $  . The ratio   $ B_{(s)}\\rightarrow h\\chi_{c0}\\rightarrow h\\pi^+\\pi^-(K^+K^-) $   between the decays   $ B_{(s)}\\rightarrow h\\chi_{c0}\\rightarrow h\\pi^+\\pi^-(K^+K^-) $     $ B_{(s)}\\rightarrow h\\chi_{c0}\\rightarrow h\\pi^+\\pi^-(K^+K^-) $   and   $ B_{(s)}\\rightarrow h\\chi_{c0}\\rightarrow h\\pi^+\\pi^-(K^+K^-) $   and the distribution of branching ratios for different decay modes in invariant mass are considered in this study."
    }
  ], 
  "imprints": [
    {
      "date": "2023-04-01", 
      "publisher": "IOP"
    }
  ]
}