ϒ(3S) and χb(3P) production and polarization in the NRQCD with kT–factorization

The ϒ(3S) production and polarization at high energies is studied in the framework of kT–factorization approach. Our consideration is based on the non-relativistic QCD formalism for bound states formation and off-shell production amplitudes for hard partonic subprocesses. The transverse momentum dep...

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Main Authors: Abdulov Nizami, Lipatov Artem
Format: Article
Language:English
Published: EDP Sciences 2019-01-01
Series:EPJ Web of Conferences
Online Access:https://www.epj-conferences.org/articles/epjconf/pdf/2019/27/epjconf_qfthep2019_03013.pdf
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spelling doaj-83e1e507804b43ebaca2e9ae429d63342021-08-02T13:35:39ZengEDP SciencesEPJ Web of Conferences2100-014X2019-01-012220301310.1051/epjconf/201922203013epjconf_qfthep2019_03013ϒ(3S) and χb(3P) production and polarization in the NRQCD with kT–factorizationAbdulov NizamiLipatov ArtemThe ϒ(3S) production and polarization at high energies is studied in the framework of kT–factorization approach. Our consideration is based on the non-relativistic QCD formalism for bound states formation and off-shell production amplitudes for hard partonic subprocesses. The transverse momentum dependent (TMD, or unintegrated) gluon densities in a proton were derived from the CiafaloniCatani-Fiorani-Marchesini (CCFM) evolution equation as well as from the Kimber–Martin–Ryskin (KMR) prescription. Treating the nonperturbative color octet transitions in terms of the mulitpole radiation theory and taking into account feed-down contributions from radiative χb(3P) decays, we extract the corresponding non-perturbative matrix elements for ϒ(3S) and χb(3P) mesons from a combined fit to ϒ(3S) transverse momenta distributions measured by the CMS and ATLAS Collaborations at the LHC energies √s = 7 and 13 TeV and central rapidities. Then we apply the extracted values to investigate the polarization parameters λθ, λφ and λθφ, which determine the ϒ(3S) spindensity matrix. Our predictions have a good agreement with the currently available data within the theoretical and experimental uncertainties.https://www.epj-conferences.org/articles/epjconf/pdf/2019/27/epjconf_qfthep2019_03013.pdf
collection DOAJ
language English
format Article
sources DOAJ
author Abdulov Nizami
Lipatov Artem
spellingShingle Abdulov Nizami
Lipatov Artem
ϒ(3S) and χb(3P) production and polarization in the NRQCD with kT–factorization
EPJ Web of Conferences
author_facet Abdulov Nizami
Lipatov Artem
author_sort Abdulov Nizami
title ϒ(3S) and χb(3P) production and polarization in the NRQCD with kT–factorization
title_short ϒ(3S) and χb(3P) production and polarization in the NRQCD with kT–factorization
title_full ϒ(3S) and χb(3P) production and polarization in the NRQCD with kT–factorization
title_fullStr ϒ(3S) and χb(3P) production and polarization in the NRQCD with kT–factorization
title_full_unstemmed ϒ(3S) and χb(3P) production and polarization in the NRQCD with kT–factorization
title_sort ϒ(3s) and χb(3p) production and polarization in the nrqcd with kt–factorization
publisher EDP Sciences
series EPJ Web of Conferences
issn 2100-014X
publishDate 2019-01-01
description The ϒ(3S) production and polarization at high energies is studied in the framework of kT–factorization approach. Our consideration is based on the non-relativistic QCD formalism for bound states formation and off-shell production amplitudes for hard partonic subprocesses. The transverse momentum dependent (TMD, or unintegrated) gluon densities in a proton were derived from the CiafaloniCatani-Fiorani-Marchesini (CCFM) evolution equation as well as from the Kimber–Martin–Ryskin (KMR) prescription. Treating the nonperturbative color octet transitions in terms of the mulitpole radiation theory and taking into account feed-down contributions from radiative χb(3P) decays, we extract the corresponding non-perturbative matrix elements for ϒ(3S) and χb(3P) mesons from a combined fit to ϒ(3S) transverse momenta distributions measured by the CMS and ATLAS Collaborations at the LHC energies √s = 7 and 13 TeV and central rapidities. Then we apply the extracted values to investigate the polarization parameters λθ, λφ and λθφ, which determine the ϒ(3S) spindensity matrix. Our predictions have a good agreement with the currently available data within the theoretical and experimental uncertainties.
url https://www.epj-conferences.org/articles/epjconf/pdf/2019/27/epjconf_qfthep2019_03013.pdf
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