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<Article>
<Journal>
<PublisherName>OICC Press</PublisherName>
<JournalTitle>Journal of Theoretical and Applied Physics</JournalTitle>
<Issn>2251-7235</Issn>
<Volume>11</Volume>
<Issue>4</Issue>
<PubDate PubStatus="epublish">
<Year>2023</Year>
<Month>11</Month>
<Day>17</Day>
</PubDate>
</Journal>
<ArticleTitle>Proof of factorization of ÏcJdocumentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt}  egin{document}$$chi _{ ext{cJ}}$$end{document} production in non-equilibrium QCD at RHIC and LHC in color singlet mechanism</ArticleTitle>
<VernacularTitle></VernacularTitle>
<FirstPage></FirstPage>
<LastPage></LastPage>
<ELocationID EIdType="doi">10.1007/s40094-017-0267-7</ELocationID>
<Language>EN</Language>
<AuthorList>
<Author>
<FirstName>OICC</FirstName>
<LastName>Press Authors</LastName>
<Affiliation>Various OICC Press Authors</Affiliation>
<Identifier Source="ORCID"></Identifier>
</Author>
</AuthorList>
<PublicationType>Journal Article</PublicationType>
<History>
<PubDate PubStatus="received">
<Year>2023</Year>
<Month>11</Month>
<Day>17</Day>
</PubDate>
</History>
<Abstract>AbstractRecently we have proved the factorization of NRQCD S-wave heavy quarkonium production at all orders in coupling constant. In this paper we extend this to prove the factorization of infrared divergences in ÏcJdocumentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$chi _{ ext{cJ}}$$end{document} production from color singlet cc¯documentclass[12pt]{minimal} usepackage{amsmath} usepackage{wasysym} usepackage{amsfonts} usepackage{amssymb} usepackage{amsbsy} usepackage{mathrsfs} usepackage{upgreek} setlength{oddsidemargin}{-69pt} egin{document}$$c{ ar{c}}$$end{document} pair in non-equilibrium QCD at RHIC and LHC at all orders in coupling constant. This can be relevant to study the quarkâgluon plasma at RHIC and LHC.</Abstract>
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<Param Name="value">Equilibrium QCD</Param>
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<Object Type="keyword">
<Param Name="value">Factorization</Param>
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<Object Type="keyword">
<Param Name="value">Gluon plasma</Param>
</Object>
<Object Type="keyword">
<Param Name="value">Heavy quarkonium</Param>
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<Param Name="value">LHC</Param>
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<Param Name="value">Non</Param>
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<Param Name="value">RHIC</Param>
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