002291437 001__ 2291437
002291437 003__ SzGeCERN
002291437 005__ 20210209110730.0
002291437 0247_ $$2DOI$$9IOP$$a10.1088/1742-6596/798/1/012068
002291437 0248_ $$aoai:inspirehep.net:1519061$$pcerncds:CERN$$qINSPIRE:HEP$$qForCDS
002291437 035__ $$9http://inspirehep.net/oai2d$$aoai:inspirehep.net:1519061$$d2017-11-02T11:26:46Z$$h2017-11-03T06:05:56Z$$mmarcxml
002291437 035__ $$9Inspire$$a1519061
002291437 041__ $$aeng
002291437 100__ $$aToia, Alberica$$iINSPIRE-00020233$$uDarmstadt, GSI$$uGoethe U., Frankfurt (main)
002291437 245__ $$9IOP$$aALICE measures pA collisions: Collectivity in small systems?
002291437 260__ $$c2017
002291437 300__ $$a5 p
002291437 520__ $$9IOP$$aProton-nucleus collisions provide a reference for heavy ion-collisions, to study the signatures deriving from the presence of a complex nuclear structure in the initial state, which confirm that the suppression of high-p (T)hadron production observed in heavy-ion collisions is a genuine effect of the hot deconfined QGP. However, several measurements of particle production in the low and intermediate momentum region indicate the presence of coherent and collective effects, already in small systems, such as the ones produced in p-Pb collisions. Measurements from proton-lead collisions at √s(NN) = 5.02 TeV obtained by the ALICE experiment at the CERN LHC will be presented and compared to p-p, A-A and d-A experimental results at different collision energies and to the available theoretical model predictions.
002291437 540__ $$3publication$$9IOP$$acc-by$$uhttp://creativecommons.org/licenses/by/3.0/
002291437 65017 $$2SzGeCERN$$aNuclear Physics - Experiment
002291437 690C_ $$aCERN
002291437 693__ $$aCERN LHC$$eALICE
002291437 710__ $$gALICE
002291437 773__ $$c012068$$n1$$pJ. Phys.: Conf. Ser.$$v798$$wC16-10-10.2$$y2017
002291437 960__ $$a13
002291437 962__ $$b2217171$$k012068$$nmoscow20161010
002291437 980__ $$aARTICLE
002291437 980__ $$aConferencePaper
002291437 999C5 $$01190545$$9refextract$$adoi:10.1103/PhysRevLett.110.032301$$cALICE Collaboration$$mCrossref:$$o1$$sPhys.Rev.Lett.,110,032301$$y2013
002291437 999C5 $$01295687$$9refextract$$adoi:10.1140/epjc/s10052-014-3054-5$$cALICE Collaboration$$mCrossref:$$o2$$sEur.Phys.J.,C74,3054$$y2014
002291437 999C5 $$01296081$$9refextract$$adoi:10.1103/PhysRevLett.113.232301$$cALICE Collaboration$$mCrossref:$$o3$$sPhys.Rev.Lett.,113,232301$$y2014
002291437 999C5 $$01346963$$9refextract$$adoi:10.1016/j.physletb.2015.07.054$$cALICE Collaboration$$mCrossref:$$o4$$sPhys.Lett.,B749,68-81$$y2015
002291437 999C5 $$01084729$$9refextract$$adoi:10.1016/j.physletb.2012.02.077$$cCMS Collaboration$$mCrossref:$$o5$$sPhys.Lett.,B710,256$$y2012
002291437 999C5 $$01116412$$9refextract$$adoi:10.1016/j.physletb.2012.07.025$$cCMS Collaboration$$mCrossref:$$o6$$sPhys.Lett.,B715,66$$y2012
002291437 999C5 $$01322726$$9refextract$$cCMS Collaboration$$mPreprint:$$o7$$rarXiv:1410.4825$$rarXiv:1410.4825
002291437 999C5 $$01127497$$9refextract$$adoi:10.1016/j.physletb.2013.01.051$$cALICE Collaboration$$mCrossref:$$o8$$sPhys.Lett.,B720,52$$y2013
002291437 999C5 $$01251898$$9refextract$$cALICE Collaboration$$o9$$sJHEP,1402,073$$y2014
002291437 999C5 $$01335350$$9refextract$$adoi:10.1103/PhysRevC.91.064905$$cALICE Collaboration$$mCrossref:$$o10$$sPhys.Rev.,C91,064905$$y2015
002291437 999C5 $$01241423$$9refextract$$adoi:10.1016/j.physletb.2013.10.054$$cALICE Collaboration$$mCrossref:$$o11$$sPhys.Lett.,B727,371$$y2013
002291437 999C5 $$01206610$$9refextract$$adoi:10.1016/j.physletb.2013.01.012$$cALICE Collaboration$$mCrossref:$$o12$$sPhys.Lett.,B719,29-41$$y2013
002291437 999C5 $$9refextract$$cALICE Collaboration$$o13$$sPhys.Lett.,B726,16477$$y2013
002291437 999C5 $$01471838$$9refextract$$cALICE Collaboration$$mPreprint:$$o14$$rarXiv:1606.07424$$rarXiv:1606.07424$$y2016