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002233036 003__ SzGeCERN
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002233036 0247_ $$2DOI$$a10.22323/1.282.0360
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002233036 037__ $$aCMS-CR-2016-310
002233036 035__ $$9Inspire$$a1596549
002233036 041__ $$aeng
002233036 100__ $$aSun, Jian$$iINSPIRE-00338985$$jCCID-735835$$uPurdue U.
002233036 245__ $$aHeavy Flavor Production in Heavy Ion Collisions at CMS
002233036 260__ $$c2016
002233036 269__ $$aGeneva$$bCERN$$c03 Nov 2016
002233036 300__ $$a7 p
002233036 520__ $$aStudies of Heavy flavor production are of great interest in heavy ion collisions. In the produced medium, the binding potential between a quark and antiquark in quarkonium is screened by surrounding light quarks and antiquarks. Thus, the various quarkonium states are expected to be melt at different temperatures depending on their binding energies, which allows us to characterize the QCD phase transition. In addition, open heavy flavor production are relevant for flavor-dependence of the in-medium parton energy loss. In QCD, gluons are expected to lose more energy compared to quarks when passing through the QGP due to the larger color charge. Compared to light quarks, heavy quarks are expected to lose less radiative energy because gluon radiation is suppressed at angles smaller than the ratio of the quark mass to its energy. This dead cone effect (and its disappearance at high transverse momentum) can be studied using open heavy flavor mesons and heavy flavor tagged jets. With CMS detector, quarkonia, open heavy flavor meson and heavy flavor tagged jet spectra are studied with high precision. In this talk, recent results from pp, pPb and PbPb at 2.76 and 5.02 TeV collisions are presented.
002233036 540__ $$3Preprint$$aCC-BY-4.0
002233036 595__ $$aCERN EDS
002233036 65017 $$2SzGeCERN$$aDetectors and Experimental Techniques
002233036 6531_ $$9CMS$$aHeavyIons
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002233036 690C_ $$aPUBLCMS
002233036 693__ $$aCERN LHC$$eCMS
002233036 710__ $$5PH
002233036 710__ $$gCMS Collaboration
002233036 773__ $$c360$$pPoS$$vICHEP2016$$wC16-08-03$$y2016
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