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Title: Event Patterns Extracted from Transverse Momentum and Rapidity Spectra of Z Bosons and Quarkonium States Produced in pp and Pb-Pb Collisions at LHC

Abstract

Transverse momentum ( p T ) and rapidity ( y ) spectra of Z bosons and quarkonium states (some charmonium c c ¯ mesons such as J / ψ and ψ ( 2 S ) and some bottomonium b b ¯ mesons such as Υ ( 1 S ) , Υ ( 2 S ) , and Υ ( 3 S ) ) produced in proton-proton (pp) and lead-lead (Pb-Pb) collisions at the large hadron collider (LHC) are uniformly described by a hybrid model of two-component Erlang distribution for p T spectrum and two-component Gaussian distribution for y spectrum. The former distribution results from a multisource thermal model, and the latter one results from the revised Landau hydrodynamic model. The modelling results are in agreement with the experimental data measured in pp collisions at center-of-mass energies s = 2.76 and 7 TeV and in Pb-Pb collisions at center-of-mass energy per nucleon pair s N N = 2.76 TeV. Based on the parameter values extracted from p T and y spectra, the event patterns (particle scatter plots) in two-dimensional p T - y space and in three-dimensional velocity space are obtained.

Authors:
ORCiD logo [1]; ORCiD logo [1];  [2]
  1. Shanxi Univ., Taiyuan (China). Inst. of Theoretical Physics
  2. Stony Brook Univ., NY (United States). Dept. of Chemistry. Dept. of Physics
Publication Date:
Research Org.:
Stony Brook Univ., NY (United States); Shanxi Univ., Taiyuan (China)
Sponsoring Org.:
USDOE Office of Science (SC), Nuclear Physics (NP); National Natural Science Foundation of China (NSFC)
OSTI Identifier:
1362011
Grant/Contract Number:  
FG02-87ER40331; 11575103
Resource Type:
Accepted Manuscript
Journal Name:
Advances in High Energy Physics
Additional Journal Information:
Journal Volume: 2016; Journal ID: ISSN 1687-7357
Publisher:
Hindawi
Country of Publication:
United States
Language:
English
Subject:
72 PHYSICS OF ELEMENTARY PARTICLES AND FIELDS

Citation Formats

Chen, Ya-Hui, Liu, Fu-Hu, and Lacey, Roy A. Event Patterns Extracted from Transverse Momentum and Rapidity Spectra of Z Bosons and Quarkonium States Produced in pp and Pb-Pb Collisions at LHC. United States: N. p., 2016. Web. doi:10.1155/2016/9876253.
Chen, Ya-Hui, Liu, Fu-Hu, & Lacey, Roy A. Event Patterns Extracted from Transverse Momentum and Rapidity Spectra of Z Bosons and Quarkonium States Produced in pp and Pb-Pb Collisions at LHC. United States. https://doi.org/10.1155/2016/9876253
Chen, Ya-Hui, Liu, Fu-Hu, and Lacey, Roy A. Sat . "Event Patterns Extracted from Transverse Momentum and Rapidity Spectra of Z Bosons and Quarkonium States Produced in pp and Pb-Pb Collisions at LHC". United States. https://doi.org/10.1155/2016/9876253. https://www.osti.gov/servlets/purl/1362011.
@article{osti_1362011,
title = {Event Patterns Extracted from Transverse Momentum and Rapidity Spectra of Z Bosons and Quarkonium States Produced in pp and Pb-Pb Collisions at LHC},
author = {Chen, Ya-Hui and Liu, Fu-Hu and Lacey, Roy A.},
abstractNote = {Transverse momentum (pT) and rapidity (y) spectra of Z bosons and quarkonium states (some charmonium cc¯ mesons such as J/ψ and ψ(2S) and some bottomonium bb¯ mesons such asΥ(1S),Υ(2S), andΥ(3S)) produced in proton-proton (pp) and lead-lead (Pb-Pb) collisions at the large hadron collider (LHC) are uniformly described by a hybrid model of two-component Erlang distribution for pT spectrum and two-component Gaussian distribution for y spectrum. The former distribution results from a multisource thermal model, and the latter one results from the revised Landau hydrodynamic model. The modelling results are in agreement with the experimental data measured in pp collisions at center-of-mass energies s=2.76 and 7 TeV and in Pb-Pb collisions at center-of-mass energy per nucleon pairsNN=2.76 TeV. Based on the parameter values extracted from pT and y spectra, the event patterns (particle scatter plots) in two-dimensional pT-y space and in three-dimensional velocity space are obtained.},
doi = {10.1155/2016/9876253},
journal = {Advances in High Energy Physics},
number = ,
volume = 2016,
place = {United States},
year = {2016},
month = {10}
}

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R.</span> </li> <li> Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment, Vol. 355, Issue 2-3</li> <li> <span class="text-muted related-url">DOI: <a href="https://doi.org/10.1016/0168-9002(94)01112-5" class="text-muted" target="_blank" rel="noopener noreferrer">10.1016/0168-9002(94)01112-5<span class="fa fa-external-link" aria-hidden="true"></span></a></span> </li> </ul> <hr/> </div> </div> <div class="pagination-container small"> <a class="pure-button prev page" href="#" rel="prev"><span class="sr-only">Previous Page</span><span class="fa fa-angle-left"></span></a> <ul class="pagination d-inline-block" style="padding-left:.2em;"></ul> <a class="pure-button next page" href="#" rel="next"><span class="sr-only">Next Page</span><span class="fa fa-angle-right"></span></a> </div> </div> </div> <div class="col-sm-3 order-sm-3"> <ul class="nav nav-stacked"> <li class="active"><a href="" class="reference-type-filter tab-nav" data-tab="biblio-references" data-filter="type" data-pattern="*"><span class="fa fa-angle-right"></span> All References</a></li> <li class="small" style="margin-left:.75em; 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margin-top: 0.5em; padding-left: 0; line-height:1.8em;"> <li> <span style="color:#5C7B2D;"> Chen, Ya-Hui; Liu, Fu-Hu; Fakhraddin, Sakina</span> </li> <li> Journal of Physics G: Nuclear and Particle Physics, Vol. 44, Issue 2</li> <li> <span class="text-muted related-url">DOI: <a href="https://doi.org/10.1088/1361-6471/aa51f1" class="text-muted" target="_blank" rel="noopener noreferrer">10.1088/1361-6471/aa51f1<span class="fa fa-external-link" aria-hidden="true"></span></a></span> </li> </ul> <hr/> </div> </div> <div class="pagination-container small"> <a class="pure-button prev page" href="#" rel="prev"><span class="sr-only">Previous Page</span><span class="fa fa-angle-left"></span></a> <ul class="pagination d-inline-block" style="padding-left:.2em;"></ul> <a class="pure-button next page" href="#" rel="next"><span class="sr-only">Next Page</span><span class="fa fa-angle-right"></span></a> </div> </div> </div> <div class="col-sm-3 order-sm-3"> <ul class="nav nav-stacked"> <li class="active"><a href="" class="reference-type-filter tab-nav" data-filter="type" data-pattern="*"><span class="fa fa-angle-right"></span> All Cited By</a></li> <li class="small" style="margin-left:.75em; 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float:none;">[ × clear filter / sort ]</a> </div> <input type="submit" id="sort_submit_citations" name="submit" aria-label="submit" style="display: none;"/> </form> </div> </div> </div> </section> <section id="biblio-related" class="tab-content tab-content-sec " data-tab="biblio"> <div class="row"> <div class="col-sm-9 order-sm-9"> <section id="biblio-similar" class="tab-content tab-content-sec active" data-tab="related"> <div class="padding"> <p class="lead text-muted" style="font-size: 18px; margin-top:0px;">Similar Records in DOE PAGES and OSTI.GOV collections:</p> <aside> <ul class="item-list" itemscope itemtype="http://schema.org/ItemList" style="padding-left:0; list-style-type: none;"> <li> <div class="article item document" itemprop="itemListElement" itemscope itemtype="http://schema.org/WebPage"><meta itemprop="position" content="1" /><div class="item-info"> <h2 class="title" itemprop="name headline"><a href="/pages/biblio/1437810-production-he-pbpb-collisions-nn-tev-lhc" itemprop="url">Production of 4He and 4 <math><mover> <mrow> <mrow> <mi mathvariant="normal"> He </mi> </mrow> </mrow> <mo> ‾ </mo> </mover> </math> in Pb–Pb collisions at <math><msqrt> <mrow> <msub> <mrow> <mi> s </mi> </mrow> <mrow> <mi mathvariant="normal"> NN </mi> </mrow> </msub> </mrow> </msqrt> <mo> = </mo> <mn> 2.76 </mn> <mspace></mspace> <mtext> TeV </mtext> </math> at the LHC</a></h2> <div class="metadata"> <small class="text-muted" style="text-transform:uppercase;display:block;line-height:2.5em;">Journal Article</small><span class="authors"> <span class="author">Acharya, S.</span> ; <span class="author">Adamová, D.</span> ; <span class="author">Adolfsson, J.</span> ; <span class="author">...</span> <span class="text-muted pubdata"> - Nuclear Physics. A</span> </span> </div> <div class="abstract">Resul<a href='#' onclick='$(this).hide().next().show().next().show();return false;' style='margin-left:10px;'>more »</a><span style='display:none;'> ts on the production of <sup>4</sup>He and <math> <mmultiscripts> <mrow> <mover> <mrow> <mrow> <mi mathvariant="normal"> He </mi> </mrow> </mrow> <mo> ¯ </mo> </mover> </mrow> <mprescripts></mprescripts> <mrow> <mn> 4 </mn> </mrow> </mmultiscripts> </math> nuclei in Pb–Pb collisions at <math> <msqrt> <mrow> <msub> <mrow> <mi> s </mi> </mrow> <mrow> <mi mathvariant="normal"> NN </mi> </mrow> </msub> </mrow> </msqrt><mo> = </mo><mn> 2.76 </mn><mspace></mspace><mtext> TeV </mtext> </math> in the rapidity range <math> <mo> | </mo><mi> y </mi><mo> | </mo><mo> < </mo><mn> 1 </mn> </math>, using the ALICE detector, are presented in this paper. The rapidity densities corresponding to 0–10% central events are found to be <math> <mi mathvariant="normal"> d </mi><mi> N </mi><mo> / </mo><mi mathvariant="normal"> d </mi><msub> <mrow> <mi> y </mi> </mrow> <mrow> <mmultiscripts> <mrow> <mi mathvariant="normal"> He </mi> </mrow> <mprescripts></mprescripts> <mrow> <mn> 4 </mn> </mrow> </mmultiscripts> </mrow> </msub><mo> = </mo><mo> ( </mo><mn> 0.8 </mn><mo> ± </mo><mn> 0.4 </mn><mspace></mspace><mo> ( </mo><mtext> stat </mtext><mo> ) </mo><mo> ± </mo><mn> 0.3 </mn><mspace></mspace><mo> ( </mo><mtext> syst </mtext><mo> ) </mo><mo> ) </mo><mo> × </mo><msup> <mrow> <mn> 10 </mn> </mrow> <mrow> <mo> - </mo> <mn> 6 </mn> </mrow> </msup> </math> and <math> <mi mathvariant="normal"> d </mi><mi> N </mi><mo> / </mo><mi mathvariant="normal"> d </mi><msub> <mrow> <mi> y </mi> </mrow> <mrow> <mmultiscripts> <mrow> <mover> <mrow> <mi mathvariant="normal"> He </mi> </mrow> <mo> ¯ </mo> </mover> </mrow> <mprescripts></mprescripts> <mrow> <mn> 4 </mn> </mrow> </mmultiscripts> </mrow> </msub><mo> = </mo><mo> ( </mo><mn> 1.1 </mn><mo> ± </mo><mn> 0.4 </mn><mspace></mspace><mo> ( </mo><mtext> stat </mtext><mo> ) </mo><mo> ± </mo><mn> 0.2 </mn><mspace></mspace><mo> ( </mo><mtext> syst </mtext><mo> ) </mo><mo> ) </mo><mo> × </mo><msup> <mrow> <mn> 10 </mn> </mrow> <mrow> <mo> - </mo> <mn> 6 </mn> </mrow> </msup> </math>, respectively. This is in agreement with the statistical thermal model expectation assuming the same chemical freeze-out temperature ( <math> <msub> <mrow> <mi> T </mi> </mrow> <mrow> <mi mathvariant="normal"> chem </mi> </mrow> </msub><mo> = </mo><mn> 156 </mn><mspace></mspace><mtext> MeV </mtext> </math>) as for light hadrons. The measured ratio of <math> <mmultiscripts> <mrow> <mover> <mrow> <mrow> <mi mathvariant="normal"> He </mi> </mrow> </mrow> <mo> ¯ </mo> </mover> </mrow> <mprescripts></mprescripts> <mrow> <mn> 4 </mn> </mrow> </mmultiscripts><msup> <mrow> <mo> / </mo> </mrow> <mrow> <mn> 4 </mn> </mrow> </msup><mrow> <mi mathvariant="normal"> He </mi> </mrow> </math> is <math> <mn> 1.4 </mn><mo> ± </mo><mn> 0.8 </mn><mspace></mspace><mo> ( </mo><mtext> stat </mtext><mo> ) </mo><mo> ± </mo><mn> 0.5 </mn><mspace></mspace><mo> ( </mo><mtext> syst </mtext><mo> ) </mo> </math>.</span><a href='#' onclick='$(this).hide().prev().hide().prev().show();return false;' style='margin-left:10px;display:none;'>« less</a></div><div class="metadata-links small clearfix text-muted" style="margin-top:15px;"> <span class="fa fa-book text-muted" aria-hidden="true"></span> Cited by 9<div class="pure-menu pure-menu-horizontal pull-right" style="width:unset;"> <ul class="pure-menu-list"> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc doi-link " href="https://doi.org/10.1016/j.nuclphysa.2017.12.004" target="_blank" rel="noopener" title="Link to document DOI" data-ostiid="1437810" data-product-type="Journal Article" data-product-subtype="PA" >https://doi.org/10.1016/j.nuclphysa.2017.12.004</a></span></li> </ul> </div> </div> </div> <div class="clearfix"></div> </div> </li> <li> <div class="article item document" itemprop="itemListElement" itemscope itemtype="http://schema.org/WebPage"><meta itemprop="position" content="2" /><div class="item-info"> <h2 class="title" itemprop="name headline"><a href="/pages/biblio/1489300-suppression-forward-rapidity-pbpb-collisions-nn-tev" itemprop="url">ϒ suppression at forward rapidity in Pb–Pb collisions at <math><msqrt> <mrow> <msub> <mrow> <mi> s </mi> </mrow> <mrow> <mi mathvariant="normal"> NN </mi> </mrow> </msub> </mrow> </msqrt> <mo> = </mo> <mn> 5.02 </mn> <mspace></mspace> <mtext> TeV </mtext> </math></a></h2> <div class="metadata"> <small class="text-muted" style="text-transform:uppercase;display:block;line-height:2.5em;">Journal Article</small><span class="authors"> <span class="author">Acharya, S.</span> ; <span class="author">Acosta, F. T.</span> ; <span class="author">Adamová, D.</span> ; <span class="author">...</span> <span class="text-muted pubdata"> - Physics Letters B</span> </span> </div> <div class="abstract">Inclusive Υ(1S)<a href='#' onclick='$(this).hide().next().show().next().show();return false;' style='margin-left:10px;'>more »</a><span style='display:none;'> and Υ(2S) production have been measured in Pb–Pb collisions at the centre-of-mass energy per nucleon–nucleon pair <math> <msqrt> <mrow> <msub> <mrow> <mi> s </mi> </mrow> <mrow> <mi mathvariant="normal"> NN </mi> </mrow> </msub> </mrow> </msqrt><mo> = </mo><mn> 5.02 </mn> </math> TeV, using the ALICE detector at the CERN LHC. The Υ mesons are reconstructed in the centre-of-mass rapidity interval <math> <mn> 2.5 </mn><mo> < </mo><mi> y </mi><mo> < </mo><mn> 4 </mn> </math> and in the transverse-momentum range <math> <msub> <mrow> <mi> p </mi> </mrow> <mrow> <mi mathvariant="normal"> T </mi> </mrow> </msub><mo> < </mo><mn> 15 </mn> </math> GeV/<em>c</em>, via their decays to muon pairs. In this Letter, we present results on the inclusive Υ(1S) nuclear modification factor <math> <msub> <mrow> <mi> R </mi> </mrow> <mrow> <mi mathvariant="normal"> AA </mi> </mrow> </msub> </math> as a function of collision centrality, transverse momentum and rapidity. The Υ(1S) and Υ(2S) <math> <msub> <mrow> <mi> R </mi> </mrow> <mrow> <mtext> AA </mtext> </mrow> </msub> </math>, integrated over the centrality range 0–90%, are <math> <mn> 0.37 </mn><mo> ± </mo><mn> 0.02 </mn><mrow> <mo> ( </mo> <mi mathvariant="normal"> stat </mi> <mo> ) </mo> </mrow><mo> ± </mo><mn> 0.03 </mn><mrow> <mo> ( </mo> <mi mathvariant="normal"> syst </mi> <mo> ) </mo> </mrow> </math> and <math> <mn> 0.10 </mn><mo> ± </mo><mn> 0.04 </mn><mrow> <mo> ( </mo> <mi mathvariant="normal"> stat </mi> <mo> ) </mo> </mrow><mo> ± </mo><mn> 0.02 </mn><mrow> <mo> ( </mo> <mi mathvariant="normal"> syst </mi> <mo> ) </mo> </mrow> </math>, respectively, leading to a ratio <math> <msubsup> <mrow> <mi> R </mi> </mrow> <mrow> <mi mathvariant="normal"> AA </mi> </mrow> <mrow> <mi mathvariant="normal"> V </mi> <mo> ( </mo> <mrow> <mn> 2S </mn> </mrow> <mo> ) </mo> </mrow> </msubsup><mo> / </mo><msubsup> <mrow> <mi> R </mi> </mrow> <mrow> <mi mathvariant="normal"> AA </mi> </mrow> <mrow> <mi mathvariant="normal"> Υ </mi> <mo> ( </mo> <mrow> <mn> 1S </mn> </mrow> <mo> ) </mo> </mrow> </msubsup> </math> of <math> <mn> 0.28 </mn><mo> ± </mo><mn> 0.12 </mn><mtext> (stat) </mtext><mo> ± </mo><mn> 0.06 </mn><mtext> (syst) </mtext> </math>. The observed Υ(1S) suppression increases with the centrality of the collision and no significant variation is observed as a function of transverse momentum and rapidity.(1S) and Υ(2S) production have been measured in Pb–Pb collisions at the centre-of-mass energy per nucleon–nucleon pair <math> <msqrt> <mrow> <msub> <mrow> <mi> s </mi> </mrow> <mrow> <mi mathvariant="normal"> NN </mi> </mrow> </msub> </mrow> </msqrt><mo> = </mo><mn> 5.02 </mn> </math> TeV, using the ALICE detector at the CERN LHC. The Υ mesons are reconstructed in the centre-of-mass rapidity interval <math> <mn> 2.5 </mn><mo> < </mo><mi> y </mi><mo> < </mo><mn> 4 </mn> </math> and in the transverse-momentum range <math> <msub> <mrow> <mi> p </mi> </mrow> <mrow> <mi mathvariant="normal"> T </mi> </mrow> </msub><mo> < </mo><mn> 15 </mn> </math> GeV/<em>c</em>, via their decays to muon pairs. In this Letter, we present results on the inclusive Υ(1S) nuclear modification factor <math> <msub> <mrow> <mi> R </mi> </mrow> <mrow> <mi mathvariant="normal"> AA </mi> </mrow> </msub> </math> as a function of collision centrality, transverse momentum and rapidity. The Υ(1S) and Υ(2S) <math> <msub> <mrow> <mi> R </mi> </mrow> <mrow> <mtext> AA </mtext> </mrow> </msub> </math>, integrated over the centrality range 0–90%, are <math> <mn> 0.37 </mn><mo> ± </mo><mn> 0.02 </mn><mrow> <mo> ( </mo> <mi mathvariant="normal"> stat </mi> <mo> ) </mo> </mrow><mo> ± </mo><mn> 0.03 </mn><mrow> <mo> ( </mo> <mi mathvariant="normal"> syst </mi> <mo> ) </mo> </mrow> </math> and <math> <mn> 0.10 </mn><mo> ± </mo><mn> 0.04 </mn><mrow> <mo> ( </mo> <mi mathvariant="normal"> stat </mi> <mo> ) </mo> </mrow><mo> ± </mo><mn> 0.02 </mn><mrow> <mo> ( </mo> <mi mathvariant="normal"> syst </mi> <mo> ) </mo> </mrow> </math>, respectively, leading to a ratio <math> <msubsup> <mrow> <mi> R </mi> </mrow> <mrow> <mi mathvariant="normal"> AA </mi> </mrow> <mrow> <mi mathvariant="normal"> Υ </mi> <mo> ( </mo> <mrow> <mn> 2S </mn> </mrow> <mo> ) </mo> </mrow> </msubsup><mo> / </mo><msubsup> <mrow> <mi> R </mi> </mrow> <mrow> <mi mathvariant="normal"> AA </mi> </mrow> <mrow> <mi mathvariant="normal"> Υ </mi> <mo> ( </mo> <mrow> <mn> 1S </mn> </mrow> <mo> ) </mo> </mrow> </msubsup> </math> of <math> <mn> 0.28 </mn><mo> ± </mo><mn> 0.12 </mn><mtext> (stat) </mtext><mo> ± </mo><mn> 0.06 </mn><mtext> (syst) </mtext> </math>. The observed Υ(1S) suppression increases with the centrality of the collision and no significant variation is observed as a function of transverse momentum and rapidity.</span><a href='#' onclick='$(this).hide().prev().hide().prev().show();return false;' style='margin-left:10px;display:none;'>« less</a></div><div class="metadata-links small clearfix text-muted" style="margin-top:15px;"> <span class="fa fa-book text-muted" aria-hidden="true"></span> Cited by 4<div class="pure-menu pure-menu-horizontal pull-right" style="width:unset;"> <ul class="pure-menu-list"> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc doi-link " href="https://doi.org/10.1016/j.physletb.2018.11.067" target="_blank" rel="noopener" title="Link to document DOI" data-ostiid="1489300" data-product-type="Journal Article" data-product-subtype="PA" >https://doi.org/10.1016/j.physletb.2018.11.067</a></span></li> </ul> </div> </div> </div> <div class="clearfix"></div> </div> </li> <li> <div class="article item document" itemprop="itemListElement" itemscope itemtype="http://schema.org/WebPage"><meta itemprop="position" content="4" /><div class="item-info"> <h2 class="title" itemprop="name headline"><a href="/pages/biblio/1525288-first-observation-forward-zbb-production-pp-collisions" itemprop="url">First observation of forward <math> <mi> Z </mi><mo> → </mo><mi> b </mi><mover> <mrow> <mi> b </mi> </mrow> <mrow> <mo> ¯ </mo> </mrow> </mover> </math> production in pp collisions at <math> <msqrt> <mrow> <mi> s </mi> </mrow> </msqrt><mo> = </mo><mn> 8 </mn><mtext>  TeV </mtext> </math></a></h2> <div class="metadata"> <small class="text-muted" style="text-transform:uppercase;display:block;line-height:2.5em;">Journal Article</small><span class="authors"> <span class="author">Aaij, R.</span> ; <span class="author">Adeva, B.</span> ; <span class="author">Adinolfi, M.</span> ; <span class="author">...</span> <span class="text-muted pubdata"> - Physics Letters. B</span> </span> </div> <div class="abstract">T<a href='#' onclick='$(this).hide().next().show().next().show();return false;' style='margin-left:10px;'>more »</a><span style='display:none;'> he decay <math> <mi> Z </mi><mo> → </mo><mi> b </mi><mover> <mrow> <mi> b </mi> </mrow> <mrow> <mo> ¯ </mo> </mrow> </mover> </math> is reconstructed in <em>pp</em> collision data, corresponding to 2 fb<sup>-1</sup> of integrated luminosity, collected by the LHCb experiment at a centre-of-mass energy of <math> <msqrt> <mrow> <mi> s </mi> </mrow> </msqrt><mo> = </mo><mn> 8 </mn> </math> eV. he product of the <em>Z</em> production cross-section and the <math> <mi> Z </mi><mo> → </mo><mi> b </mi><mover> <mrow> <mi> b </mi> </mrow> <mrow> <mo> ¯ </mo> </mrow> </mover> </math> branching fraction is measured for candidates in the fiducial region defined by two particle-level <em>b</em>-quark jets with pseudorapidities in the range <math> <mn> 2.2 </mn><mo> < </mo><mi> η </mi><mo> < </mo><mn> 4.2 </mn> </math>, with transverse momenta <math> <msub> <mrow> <mi> p </mi> </mrow> <mrow> <mi mathvariant="normal"> </mi> </mrow> </msub><mo> > </mo><mn> 20 </mn> </math> GeV and dijet invariant mass in the range <math> <mn> 45 </mn><mo> < </mo><msub> <mrow> <mi> m </mi> </mrow> <mrow> <mi> j </mi> <mi> j </mi> </mrow> </msub><mo> < </mo><mn> 165 </mn> </math> GeV. From a signal yield of <math> <mn> 5462 </mn><mo> ± </mo><mn> 763 </mn> </math> <math> <mi> Z </mi><mo> → </mo><mi> b </mi><mover> <mrow> <mi> b </mi> </mrow> <mrow> <mo> ¯ </mo> </mrow> </mover> </math> events, where the uncertainty is statistical, a production cross-section times branching fraction of <math> <mn> 332 </mn><mo> ± </mo><mn> 46 </mn><mo> ± </mo><mn> 59 </mn> </math> pb is obtained, where the first uncertainty is statistical and the second systematic. he measured significance of the signal yield is 6.0 standard deviations. his measurement represents the first observation of the <math> <mi> Z </mi><mo> → </mo><mi> b </mi><mover> <mrow> <mi> b </mi> </mrow> <mrow> <mo> ¯ </mo> </mrow> </mover> </math> production in the forward region of <em>pp</em> collisions.</span><a href='#' onclick='$(this).hide().prev().hide().prev().show();return false;' style='margin-left:10px;display:none;'>« less</a></div><div class="metadata-links small clearfix text-muted" style="margin-top:15px;"> <span class="fa fa-book text-muted" aria-hidden="true"></span> Cited by 2<div class="pure-menu pure-menu-horizontal pull-right" style="width:unset;"> <ul class="pure-menu-list"> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc doi-link " href="https://doi.org/10.1016/j.physletb.2017.11.066" target="_blank" rel="noopener" title="Link to document DOI" data-ostiid="1525288" data-product-type="Journal Article" data-product-subtype="AM" >https://doi.org/10.1016/j.physletb.2017.11.066</a></span></li> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc fulltext-link " href="/pages/servlets/purl/1525288" title="Link to document media" target="_blank" rel="noopener" data-ostiid="1525288" data-product-type="Journal Article" data-product-subtype="AM" >Full Text Available</a></span></li> </ul> </div> </div> </div> <div class="clearfix"></div> </div> </li> <li> <div class="article item document" itemprop="itemListElement" itemscope itemtype="http://schema.org/WebPage"><meta itemprop="position" content="5" /><div class="item-info"> <h2 class="title" itemprop="name headline"><a href="/pages/biblio/1716827-observable-signatures-initial-state-momentum-anisotropies-nuclear-collisions" itemprop="url">Observable signatures of initial state momentum anisotropies in nuclear collisions</a></h2> <div class="metadata"> <small class="text-muted" style="text-transform:uppercase;display:block;line-height:2.5em;">Journal Article</small><span class="authors"> <span class="author">Giacalone, Giuliano</span> ; <span class="author">Schenke, Björn</span> ; <span class="author">Shen, Chun</span> <span class="text-muted pubdata"> - Physical Review Letters</span> </span> </div> <div class="abstract">In<a href='#' onclick='$(this).hide().next().show().next().show();return false;' style='margin-left:10px;'>more »</a><span style='display:none;'> this work, we show that the correlation between the elliptic momentum anisotropy <math> <msub> <mi> v </mi> <mn> 2 </mn> </msub> </math> and the average transverse momentum <math> <mo> [ </mo><msub> <mi> p </mi> <mi> T </mi> </msub><mo> ] </mo> </math> at fixed multiplicity in small system nuclear collisions carries information on the origin of the observed momentum anisotropy. A calculation using a hybrid IP-Glasma+music+UrQMD model that includes contributions from final state response to the initial geometry as well as initial state momentum anisotropies of the color glass condensate predicts a characteristic sign change of the correlator <math> <mover> <mi> ρ </mi> <mo> ^ </mo> </mover><mo> ( </mo><msubsup> <mi> v </mi> <mn> 2 </mn> <mn> 2 </mn> </msubsup><mo> , </mo><mo> [ </mo><msub> <mi> p </mi> <mi> T </mi> </msub><mo> ] </mo><mo> ) </mo> </math> as a function of charged particle multiplicity in <math> <mi> p </mi><mo> + </mo><mtext> Au </mtext> </math> and <math> <mi> d </mi><mo> + </mo><mtext> Au </mtext> </math> collisions at <math> <msqrt> <mi> s </mi> </msqrt><mo> = </mo><mn> 200 </mn><mtext> </mtext><mtext> </mtext><mi> GeV </mi> </math>, and <math> <mi> p </mi><mo> + </mo><mi> Pb </mi> </math> collisions at <math> <msqrt> <mi> s </mi> </msqrt><mo> = </mo><mn> 5.02 </mn><mtext> </mtext><mtext> </mtext><mi> TeV </mi> </math>. This sign change is absent in calculations without initial state momentum anisotropies. The model further predicts a qualitative difference between the centrality dependence of <math> <mover> <mi> ρ </mi> <mo> ^ </mo> </mover><mo> ( </mo><msubsup> <mi> v </mi> <mn> 2 </mn> <mn> 2 </mn> </msubsup><mo> , </mo><mo> [ </mo><msub> <mi> p </mi> <mi> T </mi> </msub><mo> ] </mo><mo> ) </mo> </math> in <math> <mrow> <mi> Au </mi> <mo> + </mo> <mrow> <mi> Au </mi> </mrow> </mrow> </math> collisions at <math> <msqrt> <mi> s </mi> </msqrt><mo> = </mo><mn> 200 </mn><mtext> </mtext><mtext> </mtext><mi> GeV </mi> </math> and <math> <mrow> <mi> Pb </mi> <mo> + </mo> <mrow> <mi> Pb </mi> </mrow> </mrow> </math> collisions at <math> <msqrt> <mi> s </mi> </msqrt><mo> = </mo><mn> 5.02 </mn><mtext> </mtext><mtext> </mtext><mi> TeV </mi> </math>, with only the latter showing a sign change in peripheral events. Predictions for <math> <mrow> <mi mathvariant="normal"> O </mi> <mo> + </mo> <mi mathvariant="normal"> O </mi> </mrow> </math> collisions at different collision energy show a similar behavior. Experimental observation of these distinct qualitative features of <math> <mover> <mi> ρ </mi> <mo> ^ </mo> </mover><mo> ( </mo><msubsup> <mi> v </mi> <mn> 2 </mn> <mn> 2 </mn> </msubsup><mo> , </mo><mo> [ </mo><msub> <mi> p </mi> <mi> T </mi> </msub><mo> ] </mo><mo> ) </mo> </math> in small and large systems would constitute strong evidence for the presence and importance of initial state momentum anisotropies predicted by the color glass condensate effective theory.</span><a href='#' onclick='$(this).hide().prev().hide().prev().show();return false;' style='margin-left:10px;display:none;'>« less</a></div><div class="metadata-links small clearfix text-muted" style="margin-top:15px;"> <div class="pure-menu pure-menu-horizontal pull-right" style="width:unset;"> <ul class="pure-menu-list"> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc doi-link " href="https://doi.org/10.1103/PhysRevLett.125.192301" target="_blank" rel="noopener" title="Link to document DOI" data-ostiid="1716827" data-product-type="Journal Article" data-product-subtype="AM" >https://doi.org/10.1103/PhysRevLett.125.192301</a></span></li> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc fulltext-link " href="/pages/servlets/purl/1716827" title="Link to document media" target="_blank" rel="noopener" data-ostiid="1716827" data-product-type="Journal Article" data-product-subtype="AM" >Full Text Available</a></span></li> </ul> </div> </div> </div> <div class="clearfix"></div> </div> </li> <li> <div class="article item document" itemprop="itemListElement" itemscope itemtype="http://schema.org/WebPage"><meta itemprop="position" content="6" /><div class="item-info"> <h2 class="title" itemprop="name headline"><a href="/pages/biblio/1198154-measurement-jet-suppression-central-pbpb-collisions-nn-tev" itemprop="url">Measurement of jet suppression in central Pb–Pb collisions at <math><msqrt> <msub> <mrow> <mi> s </mi> </mrow> <mrow> <mi mathvariant="normal"> NN </mi> </mrow> </msub> </msqrt> <mo> = </mo> <mn> 2.76 </mn> <mtext> TeV </mtext> </math></a></h2> <div class="metadata"> <small class="text-muted" style="text-transform:uppercase;display:block;line-height:2.5em;">Journal Article</small><span class="authors"> <span class="author">Adam, J.</span> ; <span class="author">Adamová, D.</span> ; <span class="author">Aggarwal, M. M.</span> ; <span class="author">...</span> <span class="text-muted pubdata"> - Physics Letters B</span> </span> </div> <div class="abstract">T<a href='#' onclick='$(this).hide().next().show().next().show();return false;' style='margin-left:10px;'>more »</a><span style='display:none;'> he transverse momentum ( <math> <msub> <mrow> <mi> p </mi> </mrow> <mrow> <mi mathvariant="normal"> </mi> </mrow> </msub> </math>) spectrum and nuclear modification factor ( <math> <msub> <mrow> <mi> R </mi> </mrow> <mrow> <mi mathvariant="normal"> AA </mi> </mrow> </msub> </math>) of reconstructed jets in 0–10% and 10–30% central Pb–Pb collisions at <math> <msqrt> <msub> <mrow> <mi> s </mi> </mrow> <mrow> <mi mathvariant="normal"> NN </mi> </mrow> </msub> </msqrt><mo> = </mo><mn> 2.76 </mn><mtext> eV </mtext> </math> were measured. Jets were reconstructed using the anti- <math> <msub> <mrow> <mi> k </mi> </mrow> <mrow> <mi mathvariant="normal"> </mi> </mrow> </msub> </math> jet algorithm with a resolution parameter of <math> <mi> R </mi><mo> = </mo><mn> 0.2 </mn> </math> from charged and neutral particles, utilizing the ALICE tracking detectors and Electromagnetic Calorimeter (EMCal). he jet <math> <msub> <mrow> <mi> p </mi> </mrow> <mrow> <mi mathvariant="normal"> </mi> </mrow> </msub> </math> spectra are reported in the pseudorapidity interval of <math> <mo> | </mo><msub> <mrow> <mi> η </mi> </mrow> <mrow> <mi mathvariant="normal"> jet </mi> </mrow> </msub><mo> | </mo><mo> < </mo><mn> 0.5 </mn> </math> for <math> <mn> 40 </mn><mo> < </mo><msub> <mrow> <mi> p </mi> </mrow> <mrow> <mi mathvariant="normal"> </mi> <mo> , </mo> <mspace></mspace> <mrow> <mi mathvariant="normal"> jet </mi> </mrow> </mrow> </msub><mo> < </mo><mn> 120 </mn><mtext> GeV </mtext><mo> / </mo><mi> c </mi> </math> in 0–10% and for <math> <mn> 30 </mn><mo> < </mo><msub> <mrow> <mi> p </mi> </mrow> <mrow> <mi mathvariant="normal"> </mi> <mo> , </mo> <mspace></mspace> <mrow> <mi mathvariant="normal"> jet </mi> </mrow> </mrow> </msub><mo> < </mo><mn> 100 </mn><mtext> GeV </mtext><mo> / </mo><mi> c </mi> </math> in 10–30% collisions. Reconstructed jets were required to contain a leading charged particle with <math> <msub> <mrow> <mi> p </mi> </mrow> <mrow> <mi mathvariant="normal"> </mi> </mrow> </msub><mo> > </mo><mn> 5 </mn><mtext> GeV </mtext><mo> / </mo><mi> c </mi> </math> to suppress jets constructed from the combinatorial background in Pb–Pb collisions. he leading charged particle requirement applied to jet spectra both in pp and Pb–Pb collisions had a negligible effect on the <math> <msub> <mrow> <mi> R </mi> </mrow> <mrow> <mi mathvariant="normal"> AA </mi> </mrow> </msub> </math>. he nuclear modification factor <math> <msub> <mrow> <mi> R </mi> </mrow> <mrow> <mi mathvariant="normal"> AA </mi> </mrow> </msub> </math> was found to be <math> <mn> 0.28 </mn><mo> ± </mo><mn> 0.04 </mn> </math> in 0–10% and <math> <mn> 0.35 </mn><mo> ± </mo><mn> 0.04 </mn> </math> in 10–30% collisions, independent of <math> <msub> <mrow> <mi> p </mi> </mrow> <mrow> <mi mathvariant="normal"> </mi> <mo> , </mo> <mspace></mspace> <mrow> <mi mathvariant="normal"> jet </mi> </mrow> </mrow> </msub> </math> within the uncertainties of the measurement. he observed suppression is in fair agreement with expectations from two model calculations with different approaches to jet quenching.</span><a href='#' onclick='$(this).hide().prev().hide().prev().show();return false;' style='margin-left:10px;display:none;'>« less</a></div><div class="metadata-links small clearfix text-muted" style="margin-top:15px;"> <span class="fa fa-book text-muted" aria-hidden="true"></span> Cited by 50<div class="pure-menu pure-menu-horizontal pull-right" style="width:unset;"> <ul class="pure-menu-list"> <li class="pure-menu-item"><span class="item-info-ftlink"><a class="misc doi-link " href="https://doi.org/10.1016/j.physletb.2015.04.039" target="_blank" rel="noopener" title="Link to document DOI" data-ostiid="1198154" data-product-type="Journal Article" data-product-subtype="PA" >https://doi.org/10.1016/j.physletb.2015.04.039</a></span></li> </ul> </div> </div> </div> <div class="clearfix"></div> </div> </li> </ul> </aside> </div> </section> </div> <div class="col-sm-3 order-sm-3"> <ul class="nav nav-stacked"> <li class="active"><a class="tab-nav disabled" data-tab="related" style="color: #636c72 !important; 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