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Higher-order relativistic corrections to gluon fragmentation into spin-triplet S-wave quarkonium

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dc.contributor.authorBodwin, Geoffrey T.-
dc.contributor.authorKim, U-Rae-
dc.contributor.authorLee, Jungil-
dc.date.accessioned2021-09-06T13:48:42Z-
dc.date.available2021-09-06T13:48:42Z-
dc.date.created2021-06-15-
dc.date.issued2012-11-
dc.identifier.issn1126-6708-
dc.identifier.urihttps://scholar.korea.ac.kr/handle/2021.sw.korea/107063-
dc.description.abstractWe compute the relative-order-nu(4) contribution to gluon fragmentation into quarkonium in the S-3(1) color-singlet channel, using the nonrelativistic QCD (NRQCD) factorization approach. The QCD fragmentation process contains infrared divergences that produce single and double poles in epsilon in 4 - 2 epsilon dimensions. We devise subtractions that isolate the pole contributions, which ultimately are absorbed into long-distance NRQCD matrix elements in the NRQCD matching procedure. The matching procedure involves two-loop renormalizations of the NRQCD operators. The subtractions are integrated over the phase space analytically in 4 -2 epsilon dimensions, and the remainder is integrated over the phase-space numerically. We find that the order-nu(4) contribution is enhanced relative to the order-nu(0) contribution. However, the order-nu(4) contribution is not important numerically at the current level of precision of quarkonium-hadroproduction phenomenology. We also estimate the contribution to hadroproduction from gluon fragmentation into quarkonium in the P-3(J) color-octet channel and find that it is significant in comparison to the complete next-to-leading-order-in-as contribution in that channel.-
dc.languageEnglish-
dc.language.isoen-
dc.publisherSPRINGER-
dc.subjectANTIQUARK BOUND-STATES-
dc.subjectHEAVY QUARKONIUM-
dc.subjectJ/PSI PRODUCTION-
dc.subjectJ-PSI-
dc.subjectANNIHILATION-
dc.subjectFACTORIZATION-
dc.subjectTEVATRON-
dc.subjectDECAY-
dc.subjectNRQCD-
dc.subjectLHC-
dc.titleHigher-order relativistic corrections to gluon fragmentation into spin-triplet S-wave quarkonium-
dc.typeArticle-
dc.contributor.affiliatedAuthorLee, Jungil-
dc.identifier.doi10.1007/JHEP11(2012)020-
dc.identifier.scopusid2-s2.0-84869015583-
dc.identifier.wosid000312197800020-
dc.identifier.bibliographicCitationJOURNAL OF HIGH ENERGY PHYSICS, no.11-
dc.relation.isPartOfJOURNAL OF HIGH ENERGY PHYSICS-
dc.citation.titleJOURNAL OF HIGH ENERGY PHYSICS-
dc.citation.number11-
dc.type.rimsART-
dc.type.docTypeArticle-
dc.description.journalClass1-
dc.description.journalRegisteredClassscie-
dc.description.journalRegisteredClassscopus-
dc.relation.journalResearchAreaPhysics-
dc.relation.journalWebOfScienceCategoryPhysics, Particles & Fields-
dc.subject.keywordPlusANTIQUARK BOUND-STATES-
dc.subject.keywordPlusHEAVY QUARKONIUM-
dc.subject.keywordPlusJ/PSI PRODUCTION-
dc.subject.keywordPlusJ-PSI-
dc.subject.keywordPlusANNIHILATION-
dc.subject.keywordPlusFACTORIZATION-
dc.subject.keywordPlusTEVATRON-
dc.subject.keywordPlusDECAY-
dc.subject.keywordPlusNRQCD-
dc.subject.keywordPlusLHC-
dc.subject.keywordAuthorNLO Computations-
dc.subject.keywordAuthorHadronic Colliders-
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