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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2019-01-01
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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 |
work_keys_str_mv |
AT abdulovnizami y3sandchb3pproductionandpolarizationinthenrqcdwithktfactorization AT lipatovartem y3sandchb3pproductionandpolarizationinthenrqcdwithktfactorization |
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