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  "authors": [
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "Department of Physics, Chongqing University, Chongqing, 401331, People\u2019s Republic of China", 
          "organization": "Chongqing University"
        }, 
        {
          "country": "China", 
          "value": "Chongqing Key Laboratory for Strongly Coupled Physics, Chongqing University, Chongqing, 401331, People\u2019s Republic of China", 
          "organization": "Chongqing University"
        }
      ], 
      "surname": "Zhan", 
      "email": "zhanxj@cqu.edu.cn", 
      "full_name": "Zhan, Xi-Jie", 
      "given_names": "Xi-Jie"
    }, 
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "Department of Physics, Chongqing University, Chongqing, 401331, People\u2019s Republic of China", 
          "organization": "Chongqing University"
        }, 
        {
          "country": "China", 
          "value": "Chongqing Key Laboratory for Strongly Coupled Physics, Chongqing University, Chongqing, 401331, People\u2019s Republic of China", 
          "organization": "Chongqing University"
        }
      ], 
      "surname": "Wu", 
      "email": "wuxg@cqu.edu.cn", 
      "full_name": "Wu, Xing-Gang", 
      "given_names": "Xing-Gang"
    }, 
    {
      "affiliations": [
        {
          "country": "China", 
          "value": "Department of Physics, Chongqing University, Chongqing, 401331, People\u2019s Republic of China", 
          "organization": "Chongqing University"
        }, 
        {
          "country": "China", 
          "value": "Chongqing Key Laboratory for Strongly Coupled Physics, Chongqing University, Chongqing, 401331, People\u2019s Republic of China", 
          "organization": "Chongqing University"
        }
      ], 
      "surname": "Zheng", 
      "email": "zhengxc@cqu.edu.cn", 
      "full_name": "Zheng, Xu-Chang", 
      "given_names": "Xu-Chang"
    }
  ], 
  "titles": [
    {
      "source": "Springer", 
      "title": "Inclusive J/\u03c8 photoproduction at the ILC within the framework of non-relativistic QCD"
    }
  ], 
  "dois": [
    {
      "value": "10.1007/JHEP09(2022)050"
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  "publication_info": [
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      "page_end": "13", 
      "journal_title": "Journal of High Energy Physics", 
      "material": "article", 
      "journal_volume": "2022", 
      "artid": "JHEP09(2022)050", 
      "year": 2022, 
      "page_start": "1", 
      "journal_issue": "9"
    }
  ], 
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    "method": "Springer", 
    "submission_number": "4429515683eb11ed93fbd61508239648"
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  "page_nr": [
    13
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  "license": [
    {
      "url": "https://creativecommons.org/licenses//by/4.0", 
      "license": "CC-BY-4.0"
    }
  ], 
  "copyright": [
    {
      "holder": "The Author(s)", 
      "year": "2022"
    }
  ], 
  "control_number": "72506", 
  "record_creation_date": "2022-09-07T06:30:05.500249", 
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      "primary": "Journal of High Energy Physics"
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  "arxiv_eprints": [
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      "value": "2207.01763"
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  ], 
  "abstracts": [
    {
      "source": "Springer", 
      "value": "Based on the non-relativistic quantum chromodynamics factorization framework, we study the inclusive J/\u03c8 photoproduction at the future high energy e + e  \u2212  collider, International Linear Collider(ILC), where the initial photons come from the back-scattering of laser and electron (positron). The intermediate states,   <math> <mi>c</mi> <mover> <mi>c</mi> <mo>\u00af</mo> </mover> </math>  $$ c\\overline{c} $$ (3   <math> <msubsup> <mi>S</mi> <mn>1</mn> <mfenced> <mn>1</mn> </mfenced> </msubsup> </math>  $$ {S}_1^{\\left[\\mathbf{1}\\right]} $$ ,1   <math> <msubsup> <mi>S</mi> <mn>0</mn> <mfenced> <mn>8</mn> </mfenced> </msubsup> </math>  $$ {S}_0^{\\left[\\mathbf{8}\\right]} $$ ,3   <math> <msubsup> <mi>S</mi> <mn>1</mn> <mfenced> <mn>8</mn> </mfenced> </msubsup> </math>  $$ {S}_1^{\\left[\\mathbf{8}\\right]} $$ , 3   <math> <msubsup> <mi>P</mi> <mrow> <mn>0</mn> <mo>,</mo> <mn>1</mn> <mo>,</mo> <mn>2</mn> </mrow> <mfenced> <mn>8</mn> </mfenced> </msubsup> </math>  $$ {P}_{0,1,2}^{\\left[\\mathbf{8}\\right]} $$ ), and resolved photoproduction processes are considered. Numerical results show that the cross section of J/\u03c8 photoproduction at the ILC could be very large, and the single resolved pro- cess via   <math> <mi>c</mi> <mover> <mi>c</mi> <mo>\u00af</mo> </mover> </math>  $$ c\\overline{c} $$ (3   <math> <msubsup> <mi>S</mi> <mn>0</mn> <mfenced> <mn>8</mn> </mfenced> </msubsup> </math>  $$ {S}_0^{\\left[\\mathbf{8}\\right]} $$ ) intermediate state dominates primarily the production. We also present various kinematic distributions for J/\u03c8 photoproduction. Combining the high luminosity of the collision, J/\u03c8 photoproduction at the ILC shall provide a good platform to test the NRQCD factorization."
    }
  ], 
  "imprints": [
    {
      "date": "2022-09-06", 
      "publisher": "Springer"
    }
  ]
}