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  "authors": [
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "School of Physics, China University of Mining and Technology, Xuzhou, 221000, China", 
          "organization": "China University of Mining and Technology"
        }
      ], 
      "surname": "Li", 
      "email": "TS22180005A31@cumt.edu.cn", 
      "full_name": "Li, Na", 
      "given_names": "Na"
    }, 
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "School of Physics, China University of Mining and Technology, Xuzhou, 221000, China", 
          "organization": "China University of Mining and Technology"
        }
      ], 
      "surname": "Xing", 
      "email": "xingye_guang@cumt.edu.cn", 
      "full_name": "Xing, Ye", 
      "given_names": "Ye"
    }, 
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "School of Physics, China University of Mining and Technology, Xuzhou, 221000, China", 
          "organization": "China University of Mining and Technology"
        }, 
        {
          "country": "China", 
          "value": "Lanzhou Center for Theoretical Physics and Key Laboratory of Theoretical Physics of Gansu Province, Lanzhou University, Lanzhou, 730000, China", 
          "organization": "Lanzhou Center for Theoretical Physics and Key Laboratory of Theoretical Physics of Gansu Province, Lanzhou University"
        }
      ], 
      "surname": "Hu", 
      "email": "huxiaohui@cumt.edu.cn", 
      "full_name": "Hu, Xiao-hui", 
      "given_names": "Xiao-hui"
    }
  ], 
  "titles": [
    {
      "source": "Springer", 
      "title": "The production of charm pentaquark from B meson within SU(3) analysis"
    }
  ], 
  "dois": [
    {
      "value": "10.1140/epjc/s10052-023-12188-1"
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      "page_end": "20", 
      "journal_title": "European Physical Journal C", 
      "material": "article", 
      "journal_volume": "83", 
      "artid": "s10052-023-12188-1", 
      "year": 2023, 
      "page_start": "1", 
      "journal_issue": "11"
    }
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    "submission_number": "202ab3aaeb2111eeae4696b6a0e1ccbd"
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      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
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  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2023"
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  "control_number": "81343", 
  "record_creation_date": "2023-11-08T03:30:19.326209", 
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  "abstracts": [
    {
      "source": "Springer", 
      "value": "We study the masses and production modes of pentaquark with the quark constituent  $$c\\bar{q}qqq$$  <math> <mrow> <mi>c</mi> <mover> <mrow> <mi>q</mi> </mrow> <mrow> <mo>\u00af</mo> </mrow> </mover> <mi>q</mi> <mi>q</mi> <mi>q</mi> </mrow> </math>  , by the tridiquark-diquark model and systematical light flavor quark symmetry SU(3) analysis. The mass spectrums show that the S-wave singly charm pentaquark  $$c{\\bar{n}}nnn,~c{\\bar{s}}ssn,~c{\\bar{n}}ssn$$  <math> <mrow> <mi>c</mi> <mover> <mrow> <mi>n</mi> </mrow> <mrow> <mo>\u00af</mo> </mrow> </mover> <mi>n</mi> <mi>n</mi> <mi>n</mi> <mo>,</mo> <mspace width=\"3.33333pt\"></mspace> <mi>c</mi> <mover> <mrow> <mi>s</mi> </mrow> <mrow> <mo>\u00af</mo> </mrow> </mover> <mi>s</mi> <mi>s</mi> <mi>n</mi> <mo>,</mo> <mspace width=\"3.33333pt\"></mspace> <mi>c</mi> <mover> <mrow> <mi>n</mi> </mrow> <mrow> <mo>\u00af</mo> </mrow> </mover> <mi>s</mi> <mi>s</mi> <mi>n</mi> </mrow> </math>   and  $$c{\\bar{n}}snn$$  <math> <mrow> <mi>c</mi> <mover> <mrow> <mi>n</mi> </mrow> <mrow> <mo>\u00af</mo> </mrow> </mover> <mi>s</mi> <mi>n</mi> <mi>n</mi> </mrow> </math>    $$(n=u,d)$$  <math> <mrow> <mo>(</mo> <mi>n</mi> <mo>=</mo> <mi>u</mi> <mo>,</mo> <mi>d</mi> <mo>)</mo> </mrow> </math>   are above their strong decay thresholds, while  $$c{\\bar{s}} nnn$$  <math> <mrow> <mi>c</mi> <mover> <mrow> <mi>s</mi> </mrow> <mrow> <mo>\u00af</mo> </mrow> </mover> <mi>n</mi> <mi>n</mi> <mi>n</mi> </mrow> </math>   and  $$c\\bar{s} snn$$  <math> <mrow> <mi>c</mi> <mover> <mrow> <mi>s</mi> </mrow> <mrow> <mo>\u00af</mo> </mrow> </mover> <mi>s</mi> <mi>n</mi> <mi>n</mi> </mrow> </math>   with parity  $$\\frac{1}{2}^-$$  <math> <msup> <mfrac> <mn>1</mn> <mn>2</mn> </mfrac> <mo>-</mo> </msup> </math>   are below their strong decay thresholds, which imply the possibility of stable states. Furthermore, we discuss the production of the concerned 15 states from B meson, the analysis within SU(3) symmetry yields the golden channels of production process,  $${\\overline{B}}^0_s\\rightarrow F_{\\bar{s}udd}^{+} {\\overline{p}},\\ B^-\\rightarrow F_{\\bar{u}dds}^{-} {\\overline{\\Lambda }}^0$$  <math> <mrow> <msubsup> <mrow> <mover> <mi>B</mi> <mo>\u00af</mo> </mover> </mrow> <mi>s</mi> <mn>0</mn> </msubsup> <mo>\u2192</mo> <msubsup> <mi>F</mi> <mrow> <mover> <mrow> <mi>s</mi> </mrow> <mrow> <mo>\u00af</mo> </mrow> </mover> <mi>u</mi> <mi>d</mi> <mi>d</mi> </mrow> <mo>+</mo> </msubsup> <mover> <mi>p</mi> <mo>\u00af</mo> </mover> <mo>,</mo> <mspace width=\"4pt\"></mspace> <msup> <mi>B</mi> <mo>-</mo> </msup> <mo>\u2192</mo> <msubsup> <mi>F</mi> <mrow> <mover> <mrow> <mi>u</mi> </mrow> <mrow> <mo>\u00af</mo> </mrow> </mover> <mi>d</mi> <mi>d</mi> <mi>s</mi> </mrow> <mo>-</mo> </msubsup> <msup> <mrow> <mover> <mi>\u039b</mi> <mo>\u00af</mo> </mover> </mrow> <mn>0</mn> </msup> </mrow> </math>  , which expected to be work worthily in b-factory."
    }
  ], 
  "imprints": [
    {
      "date": "2023-11-08", 
      "publisher": "Springer"
    }
  ]
}