002113353 001__ 2113353
002113353 003__ SzGeCERN
002113353 005__ 20220810144244.0
002113353 0247_ $$2DOI$$a10.1051/epjconf/201612006004
002113353 0248_ $$aoai:cds.cern.ch:2113353$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
002113353 035__ $$9arXiv$$aoai:arXiv.org:1512.03605
002113353 035__ $$9Inspire$$a1409296
002113353 037__ $$9arXiv$$aarXiv:1512.03605$$chep-ex
002113353 041__ $$aeng
002113353 100__ $$aMassacrier, Laure$$uOrsay, LAL$$uOrsay, IPN$$vLAL, Univ. Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, Orsay, France$$vIPNO, Univ. Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, Orsay, France
002113353 245__ $$aLHCb results from proton ion collisions
002113353 269__ $$c11 Dec 2015
002113353 260__ $$c2016-07-04
002113353 300__ $$a6 p
002113353 500__ $$9arXiv$$aproceeding of ISM2015 Conference, 4-9th October 2015, Wildbad Kreuth
002113353 520__ $$aProton-lead and lead-proton data taking during 2013 has allowed LHCb to expand its physics program to heavy ion physics. Results include the first forward measurement of Z production in proton-lead collisions as well as a measurement of the nuclear modification factor and forward-backward production of prompt and displaced J/$\psi$, $\psi$(2S) and $\Upsilon$. Angular particle correlations have also been measured for events of varying charged particle activity.
002113353 520__ $$9EDP Sciences$$aProton-lead and lead-proton data taking during 2013 has allowed LHCb to expand its physics program to heavy ion physics. Results include the first forward measurement of Z production in proton-lead collisions as well as a measurement of the nuclear modification factor and forward-backward production of prompt and displaced J/psi, psi(2S) and ϒ. Angular particle correlations have also been measured for events of varying charged particle activity.
002113353 520__ $$9arXiv$$aProton-lead and lead-proton data taking during 2013 has allowed LHCb to expand its physics program to heavy ion physics. Results include the first forward measurement of Z production in proton-lead collisions as well as a measurement of the nuclear modification factor and forward-backward production of prompt and displaced J/$\psi$, $\psi$(2S) and $\Upsilon$. Angular particle correlations have also been measured for events of varying charged particle activity.
002113353 540__ $$aarXiv nonexclusive-distrib. 1.0$$barXiv$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
002113353 540__ $$3publication$$aCC-BY-4.0
002113353 542__ $$3publication$$dThe Author(s)$$g2016
002113353 595__ $$aLANL EDS
002113353 65017 $$2arXiv$$aParticle Physics - Experiment
002113353 65027 $$2arXiv$$aNuclear Physics - Experiment
002113353 693__ $$aCERN LHC$$eLHCb
002113353 695__ $$9LANL EDS$$ahep-ex
002113353 695__ $$9LANL EDS$$anucl-ex
002113353 690C_ $$aARTICLE
002113353 690C_ $$aCERN
002113353 710__ $$gon behalf of the LHCb Collaboration
002113353 773__ $$c06004$$pEPJ Web Conf.$$v120$$wC15-10-04$$y2016
002113353 8564_ $$uhttp://arxiv.org/pdf/1512.03605.pdf$$yPreprint
002113353 8564_ $$81248354$$s681058$$uhttp://cds.cern.ch/record/2113353/files/epjconf_ismd2016_06004.pdf$$yFulltext
002113353 8564_ $$81248354$$s1669200$$uhttp://cds.cern.ch/record/2113353/files/epjconf_ismd2016_06004.pdf?subformat=pdfa$$xpdfa$$yEDP Sciences Open Access article
002113353 8564_ $$81308610$$s441753$$uhttp://cds.cern.ch/record/2113353/files/arXiv:1512.03605.pdf
002113353 8564_ $$81308608$$s9898$$uhttp://cds.cern.ch/record/2113353/files/Ups2.png$$y00005 $R_{\rm{pA}}$ (left) and $R_{\rm{FB}}$ (right) as a function of rapidity for prompt J/$\psi$ (red), J/$\psi$ from b (blue) and $\Upsilon$(1S) (black). The results are compared with theoretical predictions including energy loss and nuclear shadowing\cite{Arleo:2012rs}.
002113353 8564_ $$81308609$$s9918$$uhttp://cds.cern.ch/record/2113353/files/Ups1.png$$y00004 $R_{\rm{pA}}$ (left) and $R_{\rm{FB}}$ (right) as a function of rapidity for prompt J/$\psi$ (red), J/$\psi$ from b (blue) and $\Upsilon$(1S) (black). The results are compared with theoretical predictions including energy loss and nuclear shadowing\cite{Arleo:2012rs}.
002113353 8564_ $$81308611$$s139078$$uhttp://cds.cern.ch/record/2113353/files/Fig3b.png$$y00007 Two-particle correlation functions in the backward Pbp configuration, for low event-activity class (left) and high event-acticity class (right). The analysed pairs of prompt charged particles are selected in the $p_{\rm T}$ range 1 < $p_{\rm T}$ < 2 GeV/$c$.
002113353 8564_ $$81308612$$s140393$$uhttp://cds.cern.ch/record/2113353/files/Fig3a.png$$y00006 Two-particle correlation functions in the backward Pbp configuration, for low event-activity class (left) and high event-acticity class (right). The analysed pairs of prompt charged particles are selected in the $p_{\rm T}$ range 1 < $p_{\rm T}$ < 2 GeV/$c$.
002113353 8564_ $$81308613$$s13476$$uhttp://cds.cern.ch/record/2113353/files/Fig7b.png$$y00003 Nuclear modification factor $R_{\rm{pPb}}$ as a function of rapidity for prompt J/$\psi$ and $\psi$(2S) (left) and for J/$\psi$ and $\psi$(2S) from b-hadrons (right). Results are compared with theoretical models from Refs. \cite{Ferreiro:2013pua,delValle:2014wha} (yellow dashed line and brown band), from Ref. \cite{Albacete:2013ei} (blue band) and from Ref. \cite{Arleo:2012rs} (green solid and blue dash-dotted lines). Only the models from \cite{Ferreiro:2013pua,delValle:2014wha} are available for $\psi$(2S) from b.
002113353 8564_ $$81308614$$s38791$$uhttp://cds.cern.ch/record/2113353/files/Fig7a.png$$y00002 Nuclear modification factor $R_{\rm{pPb}}$ as a function of rapidity for prompt J/$\psi$ and $\psi$(2S) (left) and for J/$\psi$ and $\psi$(2S) from b-hadrons (right). Results are compared with theoretical models from Refs. \cite{Ferreiro:2013pua,delValle:2014wha} (yellow dashed line and brown band), from Ref. \cite{Albacete:2013ei} (blue band) and from Ref. \cite{Arleo:2012rs} (green solid and blue dash-dotted lines). Only the models from \cite{Ferreiro:2013pua,delValle:2014wha} are available for $\psi$(2S) from b.
002113353 8564_ $$81308615$$s39623$$uhttp://cds.cern.ch/record/2113353/files/Fig1a.png$$y00000 Projections of the $\psi$(2S) fit results to the dimuon invariant mass (left) and pseudo-proper time $t_{z}$ (right) in pPb forward configuration (1.5 $< \rm{y}_{CMS} <$ 4.0). For the mass projection, the total fitted function is the red line, the signal distribution is the blue dotted line and the combinatorial background is represented by the green hatched area. For the $t_{z}$ projection, the same representation is adopted and in addition the $\psi$(2S) from b-hadron signal is given by the black line.
002113353 8564_ $$81308616$$s35192$$uhttp://cds.cern.ch/record/2113353/files/Fig1c.png$$y00001 Projections of the $\psi$(2S) fit results to the dimuon invariant mass (left) and pseudo-proper time $t_{z}$ (right) in pPb forward configuration (1.5 $< \rm{y}_{CMS} <$ 4.0). For the mass projection, the total fitted function is the red line, the signal distribution is the blue dotted line and the combinatorial background is represented by the green hatched area. For the $t_{z}$ projection, the same representation is adopted and in addition the $\psi$(2S) from b-hadron signal is given by the black line.
002113353 916__ $$sn$$w201550
002113353 960__ $$a13
002113353 962__ $$b2017815$$k06004$$nkreuth20151004
002113353 980__ $$aARTICLE
002113353 980__ $$aConferencePaper