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<Article>
<Journal>
				<PublisherName>The Physics Society of Iran</PublisherName>
				<JournalTitle>Iranian Journal of Physics Research</JournalTitle>
				<Issn>1682-6957</Issn>
				<Volume>17</Volume>
				<Issue>1</Issue>
				<PubDate PubStatus="epublish">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</Journal>
<ArticleTitle>Gluon fragmentation into a vector charmonium J/psi  considering the effect of meson wave function</ArticleTitle>
<VernacularTitle>Gluon fragmentation into a vector charmonium J/psi  considering the effect of meson wave function</VernacularTitle>
			<FirstPage>81</FirstPage>
			<LastPage>90</LastPage>
			<ELocationID EIdType="pii">1236</ELocationID>
			
<ELocationID EIdType="doi">10.18869/acadpub.ijpr.17.1.81</ELocationID>
			
			<Language>FA</Language>
<AuthorList>
<Author>
					<FirstName>Seyed Mohammad</FirstName>
					<LastName>Moosavi Nejad</LastName>
<Affiliation></Affiliation>
<Identifier Source="ORCID">0000-0003-0087-291X</Identifier>

</Author>
</AuthorList>
				<PublicationType>Journal Article</PublicationType>
			<History>
				<PubDate PubStatus="received">
					<Year>2019</Year>
					<Month>11</Month>
					<Day>26</Day>
				</PubDate>
			</History>
		<Abstract>Studying the production or decay processes of heavy quarkonia (the bound state of heavy quark-antiquark) is a powerful tool to test our understanding of strong interaction dynamics and QCD theory. Fragmentation is the dominant production mechanism for heavy quarkonia with large transverse momentum. The fragmentation refers to the production process of a parton with high transverse momentum which subsequently decays into a heavy quarkonia. In all previous manuscript where the fragmentation functions of heavy mesons or baryons are calculated, authors have used the approximation of a Dirac delta function for the meson wave function. In the present paper by working in a perturbative QCD framework and by considering the effect of meson wave functions we calculate the fragmentation function of a gluon into a spin-triplet S-wave charmonium J/psi.  To consider the real aspect of meson bound state we apply a mesonic wave function which is different of Dirac delta function and is a nonrelativistic limit of the Bethe-Salpeter equation. Finally, we present our numerical results and show that how the proposed wave function improves the previous results.</Abstract>
			<OtherAbstract Language="FA">Studying the production or decay processes of heavy quarkonia (the bound state of heavy quark-antiquark) is a powerful tool to test our understanding of strong interaction dynamics and QCD theory. Fragmentation is the dominant production mechanism for heavy quarkonia with large transverse momentum. The fragmentation refers to the production process of a parton with high transverse momentum which subsequently decays into a heavy quarkonia. In all previous manuscript where the fragmentation functions of heavy mesons or baryons are calculated, authors have used the approximation of a Dirac delta function for the meson wave function. In the present paper by working in a perturbative QCD framework and by considering the effect of meson wave functions we calculate the fragmentation function of a gluon into a spin-triplet S-wave charmonium J/psi.  To consider the real aspect of meson bound state we apply a mesonic wave function which is different of Dirac delta function and is a nonrelativistic limit of the Bethe-Salpeter equation. Finally, we present our numerical results and show that how the proposed wave function improves the previous results.</OtherAbstract>
		<ObjectList>
			<Object Type="keyword">
			<Param Name="value">Gluon</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">fragmentation function</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Vector charmonium J/psi</Param>
			</Object>
			<Object Type="keyword">
			<Param Name="value">Meson wave function</Param>
			</Object>
		</ObjectList>
<ArchiveCopySource DocType="pdf">https://ijpr.iut.ac.ir/article_1236_7bccfde7714a1ebadf06c5f4cea752c1.pdf</ArchiveCopySource>
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