000291940 001__ 291940
000291940 005__ 20211110132657.0
000291940 0247_ $$2arXiv$$aarXiv:1410.8318
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000291940 037__ $$aPUBDB-2015-05674
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000291940 0881_ $$aarXiv:1410.8318
000291940 088__ $$2arXiv$$aarXiv:1410.8318
000291940 1001_ $$0INSPIRE-00242967$$aSahlmueller, Baldo$$b0
000291940 1112_ $$aPanic2014$$cHamburg$$d2014-08-25 - 2014-08-29$$gPanic2014$$wGermany
000291940 245__ $$aRecent Highlights from the PHENIX Heavy-Ion Program at RHIC
000291940 260__ $$aHamburg$$bDeutsches Elektronen-Synchrotron, DESY$$c2014
000291940 300__ $$a195-198
000291940 3367_ $$033$$2EndNote$$aConference Paper
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000291940 3367_ $$0PUB:(DE-HGF)8$$2PUB:(DE-HGF)$$aContribution to a conference proceedings$$bcontrib$$mcontrib$$s1450088426_17196
000291940 3367_ $$0PUB:(DE-HGF)15$$2PUB:(DE-HGF)$$aInternal Report$$mintrep
000291940 3367_ $$2BibTeX$$aINPROCEEDINGS
000291940 520__ $$aOver the last decade it has been established that a quark-gluon plasma (QGP) is formed in ultrarelativistic A+A collisions at RHIC energies. In recent years, detector upgrades have enabled the detailed study of this hot and dense matter. Important probes, among others, are direct photons and heavy flavor observables. Although the RHIC d+Au program was originally undertaken to study initial state and cold nuclear matter effects, recent measurements at both RHIC (d+Au) and the LHC (p+Pb) have found evidence for collective phenomena in these small systems.
000291940 536__ $$0G:(DE-HGF)POF3-611$$a611 - Fundamental Particles and Forces (POF3-611)$$cPOF3-611$$fPOF III$$x0
000291940 588__ $$aDataset connected to INSPIRE
000291940 650_7 $$2INSPIRE$$anuclear matter: effect
000291940 650_7 $$2INSPIRE$$aquark gluon: plasma
000291940 650_7 $$2INSPIRE$$adetector: upgrade
000291940 650_7 $$2INSPIRE$$aphoton: direct production
000291940 650_7 $$2INSPIRE$$aBrookhaven RHIC Coll
000291940 650_7 $$2INSPIRE$$acollective phenomena
000291940 650_7 $$2INSPIRE$$aCERN LHC Coll
000291940 650_7 $$2INSPIRE$$ainitial state
000291940 650_7 $$2INSPIRE$$aheavy quark: hadroproduction
000291940 650_7 $$2INSPIRE$$aPHENIX
000291940 650_7 $$2INSPIRE$$aheavy ion: scattering
000291940 650_7 $$2INSPIRE$$acopper
000291940 650_7 $$2INSPIRE$$agold
000291940 650_7 $$2INSPIRE$$aquarkonium: heavy
000291940 650_7 $$2INSPIRE$$aangular distribution: anisotropy
000291940 650_7 $$2INSPIRE$$aimpact parameter: dependence
000291940 650_7 $$2INSPIRE$$aexperimental results
000291940 650_7 $$2INSPIRE$$a200 GeV-cms/nucleon
000291940 693__ $$0EXP:(DE-MLZ)NOSPEC-20140101$$5EXP:(DE-MLZ)NOSPEC-20140101$$eNo specific instrument$$x0
000291940 7001_ $$0P:(DE-HGF)0$$aPHENIX Collaboration$$b1$$eCollaboration Author
000291940 773__ $$a10.3204/DESY-PROC-2014-04/318
000291940 7870_ $$0PUBDB-2015-03603$$aSchmidt, Alexander et.al.$$dHamburg : Deutsches Elektronen-Synchrotron, DESY, Hamburg, 2014$$iIsPartOf$$rDESY-PROC-2014-04$$tProceedings, 20th International Conference on Particles and Nuclei (PANIC 14)
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000291940 9201_ $$0I:(DE-H253)ATLAS-20120731$$kATLAS$$lLHC/ATLAS Experiment$$x0
000291940 9201_ $$0I:(DE-H253)CMS-20120731$$kCMS$$lLHC/CMS Experiment$$x1
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