Dielectron and heavy-quark production in inelastic and high-multiplicity proton–proton collisions at √sNN = 13 TeV
Autor(a) principal: | |
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Data de Publicação: | 2019 |
Outros Autores: | , , , |
Tipo de documento: | Artigo |
Idioma: | eng |
Título da fonte: | Repositório Institucional da UFRGS |
Texto Completo: | http://hdl.handle.net/10183/194647 |
Resumo: | The measurement of dielectron production is presented as a function of invariant mass and transverse momentum (pT) at midrapidity (|ye| <0.8) in proton–proton (pp) collisions at a centre-of-mass energy of √s=13TeV. The contributions from light-hadron decays are calculated from their measured cross sections in pp collisions at √s=7TeV or 13TeV. The remaining continuum stems from correlated semileptonic decays of heavy-flavour hadrons. Fitting the data with templates from two different MC event generators, PYTHIA and POWHEG, the charm and beauty cross sections at midrapidity are extracted for the first time at this collision energy: dσc¯ c/dy|y=0=974 ±138 (stat.) ±140 (syst.) ±214(BR)μband dσb¯ b/dy|y=0=79 ±14 (stat.) ±11 (syst.) ±5(BR)μbusing PYTHIA simulations and dσc¯ c/dy|y=0=1417 ±184 (stat.) ±204 (syst.) ±312(BR)μband dσb¯ b/dy|y=0=48 ±14 (stat.) ±7 (syst.) ±3(BR)μbfor POWHEG. These values, whose uncertainties are fully correlated between the two generators, are consistent with extrapolations from lower energies. The different results obtained with POWHEG and PYTHIA imply different kinematic correlations of the heavy-quark pairs in these two generators. Furthermore, comparisons of dielectron spectra in inelastic events and in events collected with a trigger on high charged-particle multiplicities are presented in various pTintervals. The differences are consistent with the already measured scaling of light-hadron and open-charm production at high charged-particle multiplicity as a function of pT. Upper limits for the contribution of virtual direct photons are extracted at 90% confidence level and found to be in agreement with pQCD calculations. |
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Acharya, ShreyasiGay Ducati, Maria BeatrizPereira, Luis GustavoPezzi, Rafael PerettiALICE Collaboration2019-05-28T02:36:57Z20190370-2693http://hdl.handle.net/10183/194647001088838The measurement of dielectron production is presented as a function of invariant mass and transverse momentum (pT) at midrapidity (|ye| <0.8) in proton–proton (pp) collisions at a centre-of-mass energy of √s=13TeV. The contributions from light-hadron decays are calculated from their measured cross sections in pp collisions at √s=7TeV or 13TeV. The remaining continuum stems from correlated semileptonic decays of heavy-flavour hadrons. Fitting the data with templates from two different MC event generators, PYTHIA and POWHEG, the charm and beauty cross sections at midrapidity are extracted for the first time at this collision energy: dσc¯ c/dy|y=0=974 ±138 (stat.) ±140 (syst.) ±214(BR)μband dσb¯ b/dy|y=0=79 ±14 (stat.) ±11 (syst.) ±5(BR)μbusing PYTHIA simulations and dσc¯ c/dy|y=0=1417 ±184 (stat.) ±204 (syst.) ±312(BR)μband dσb¯ b/dy|y=0=48 ±14 (stat.) ±7 (syst.) ±3(BR)μbfor POWHEG. These values, whose uncertainties are fully correlated between the two generators, are consistent with extrapolations from lower energies. The different results obtained with POWHEG and PYTHIA imply different kinematic correlations of the heavy-quark pairs in these two generators. Furthermore, comparisons of dielectron spectra in inelastic events and in events collected with a trigger on high charged-particle multiplicities are presented in various pTintervals. The differences are consistent with the already measured scaling of light-hadron and open-charm production at high charged-particle multiplicity as a function of pT. Upper limits for the contribution of virtual direct photons are extracted at 90% confidence level and found to be in agreement with pQCD calculations.application/pdfengPhysics letters. B. Amsterdam. Vol. 788 (Jan. 2019), p. 505-518Aceleradores de partículasColisões proton-protonCromodinâmica quânticaDielectron and heavy-quark production in inelastic and high-multiplicity proton–proton collisions at √sNN = 13 TeVEstrangeiroinfo:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/openAccessreponame:Repositório Institucional da UFRGSinstname:Universidade Federal do Rio Grande do Sul (UFRGS)instacron:UFRGSTEXT001088838.pdf.txt001088838.pdf.txtExtracted Texttext/plain85487http://www.lume.ufrgs.br/bitstream/10183/194647/2/001088838.pdf.txtc2aebab291a52a60cb62f1a1e120b479MD52ORIGINAL001088838.pdfTexto completo (inglês)application/pdf993148http://www.lume.ufrgs.br/bitstream/10183/194647/1/001088838.pdf8c4c545d65d315e76d2c4374044f9a5fMD5110183/1946472023-11-12 04:24:51.342711oai:www.lume.ufrgs.br:10183/194647Repositório de PublicaçõesPUBhttps://lume.ufrgs.br/oai/requestopendoar:2023-11-12T06:24:51Repositório Institucional da UFRGS - Universidade Federal do Rio Grande do Sul (UFRGS)false |
dc.title.pt_BR.fl_str_mv |
Dielectron and heavy-quark production in inelastic and high-multiplicity proton–proton collisions at √sNN = 13 TeV |
title |
Dielectron and heavy-quark production in inelastic and high-multiplicity proton–proton collisions at √sNN = 13 TeV |
spellingShingle |
Dielectron and heavy-quark production in inelastic and high-multiplicity proton–proton collisions at √sNN = 13 TeV Acharya, Shreyasi Aceleradores de partículas Colisões proton-proton Cromodinâmica quântica |
title_short |
Dielectron and heavy-quark production in inelastic and high-multiplicity proton–proton collisions at √sNN = 13 TeV |
title_full |
Dielectron and heavy-quark production in inelastic and high-multiplicity proton–proton collisions at √sNN = 13 TeV |
title_fullStr |
Dielectron and heavy-quark production in inelastic and high-multiplicity proton–proton collisions at √sNN = 13 TeV |
title_full_unstemmed |
Dielectron and heavy-quark production in inelastic and high-multiplicity proton–proton collisions at √sNN = 13 TeV |
title_sort |
Dielectron and heavy-quark production in inelastic and high-multiplicity proton–proton collisions at √sNN = 13 TeV |
author |
Acharya, Shreyasi |
author_facet |
Acharya, Shreyasi Gay Ducati, Maria Beatriz Pereira, Luis Gustavo Pezzi, Rafael Peretti ALICE Collaboration |
author_role |
author |
author2 |
Gay Ducati, Maria Beatriz Pereira, Luis Gustavo Pezzi, Rafael Peretti ALICE Collaboration |
author2_role |
author author author author |
dc.contributor.author.fl_str_mv |
Acharya, Shreyasi Gay Ducati, Maria Beatriz Pereira, Luis Gustavo Pezzi, Rafael Peretti ALICE Collaboration |
dc.subject.por.fl_str_mv |
Aceleradores de partículas Colisões proton-proton Cromodinâmica quântica |
topic |
Aceleradores de partículas Colisões proton-proton Cromodinâmica quântica |
description |
The measurement of dielectron production is presented as a function of invariant mass and transverse momentum (pT) at midrapidity (|ye| <0.8) in proton–proton (pp) collisions at a centre-of-mass energy of √s=13TeV. The contributions from light-hadron decays are calculated from their measured cross sections in pp collisions at √s=7TeV or 13TeV. The remaining continuum stems from correlated semileptonic decays of heavy-flavour hadrons. Fitting the data with templates from two different MC event generators, PYTHIA and POWHEG, the charm and beauty cross sections at midrapidity are extracted for the first time at this collision energy: dσc¯ c/dy|y=0=974 ±138 (stat.) ±140 (syst.) ±214(BR)μband dσb¯ b/dy|y=0=79 ±14 (stat.) ±11 (syst.) ±5(BR)μbusing PYTHIA simulations and dσc¯ c/dy|y=0=1417 ±184 (stat.) ±204 (syst.) ±312(BR)μband dσb¯ b/dy|y=0=48 ±14 (stat.) ±7 (syst.) ±3(BR)μbfor POWHEG. These values, whose uncertainties are fully correlated between the two generators, are consistent with extrapolations from lower energies. The different results obtained with POWHEG and PYTHIA imply different kinematic correlations of the heavy-quark pairs in these two generators. Furthermore, comparisons of dielectron spectra in inelastic events and in events collected with a trigger on high charged-particle multiplicities are presented in various pTintervals. The differences are consistent with the already measured scaling of light-hadron and open-charm production at high charged-particle multiplicity as a function of pT. Upper limits for the contribution of virtual direct photons are extracted at 90% confidence level and found to be in agreement with pQCD calculations. |
publishDate |
2019 |
dc.date.accessioned.fl_str_mv |
2019-05-28T02:36:57Z |
dc.date.issued.fl_str_mv |
2019 |
dc.type.driver.fl_str_mv |
Estrangeiro info:eu-repo/semantics/article |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
format |
article |
status_str |
publishedVersion |
dc.identifier.uri.fl_str_mv |
http://hdl.handle.net/10183/194647 |
dc.identifier.issn.pt_BR.fl_str_mv |
0370-2693 |
dc.identifier.nrb.pt_BR.fl_str_mv |
001088838 |
identifier_str_mv |
0370-2693 001088838 |
url |
http://hdl.handle.net/10183/194647 |
dc.language.iso.fl_str_mv |
eng |
language |
eng |
dc.relation.ispartof.pt_BR.fl_str_mv |
Physics letters. B. Amsterdam. Vol. 788 (Jan. 2019), p. 505-518 |
dc.rights.driver.fl_str_mv |
info:eu-repo/semantics/openAccess |
eu_rights_str_mv |
openAccess |
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application/pdf |
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