[PDF] Top 20 Pseudorapidity distributions of charged hadrons in xenon-xenon collisions at root S-NN=5.44 TeV
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Pseudorapidity distributions of charged hadrons in xenon-xenon collisions at root S-NN=5.44 TeV
... Policy Of- fice; the Fonds pour la Formation à la Recherche dans l’Indus- trie et dans l’Agriculture (FRIA-Belgium); the Agentschap voor Innovatie door Wetenschap en Technologie (IWT-Belgium); the ...“Excellence ... See full document
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Charged-particle angular correlations in XeXe collisions at root s(NN)=5.44 TeV
... (Republic of Korea); MES (Latvia); LAS (Lithuania); MOE and UM (Malaysia); BUAP, CINVESTAV, CONACYT, LNS, SEP, and UASLP-FAI (Mexico); MOS (Montenegro); MBIE (New Zealand); PAEC (Pakistan); MSHE and NSC (Poland); ... See full document
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Centrality and pseudorapidity dependence of the charged-particle multiplicity density in Xe-Xe collisions at root s(NN)=5.44 TeV
... part of the tracking system of ALICE is the Sil- icon Pixel Detector (SPD) [ 13 ] which consists of two cylindrical layers of hybrid silicon pixel ...placed at radii of ... See full document
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Centrality evolution of the charged-particle pseudorapidity density over a broad pseudorapidity range in Pb-Pb collisions at root S(NN)=2.76 TeV
... shape of the charged-particle pseudorapidity density distributions broadens only slightly toward more periph- eral events, consistent with the above ...shown in Fig. 4 versus the num- ... See full document
14
Longitudinal asymmetry and its effect on pseudorapidity distributions in Pb-Pb collisions at root s(NN)=2.76 TeV
... the pseudorapidity distributions in Pb–Pb collisions at √ s NN = ...2.76 TeV at the Large Hadron Collider are obtained with the ALICE ...because of an ... See full document
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Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at root s(NN)=5.02 TeV
... is at most 3‰ on both dN ch / d y and y — much smaller than the systematic uncertainty and η resolution of the ...Fig. 5 also shows the expected charged-particle rapid- ity densities from the ... See full document
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Charged-particle nuclear modification factors in XeXe collisions at root S-NN=5.44 TeV
... colleagues in the CERN accelerator departments for the excellent per- formance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their ... See full document
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Anisotropic Flow Of Charged Particles In Pb-pb Collisions At Root S-nn=5.02 Tev
... coincidence of signals from the V0 detector. The V0 detector is composed of two arrays of scintillator counters, V0-A and V0-C, which cover the pseudorapidity ranges ...fraction of a ... See full document
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Centrality Dependence Of Charged Jet Production In P-pb Collisions At Root(nn)-n-s=5.02 Tev
... A. Grigoras 35 , C. Grigoras 35 , V. Grigoriev 75 , A. Grigoryan 1 , S. Grigoryan 66 , B. Grinyov 3 , N. Grion 109 , J. M. Gronefeld 97 , J. F. Grosse-Oetringhaus 35 , R. Grosso 97 , F. Guber 56 , R. Guernane 71 , ... See full document
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Centrality Dependence Of The Charged-particle Multiplicity Density At Midrapidity In Pb-pb Collisions At Root(nn)-n-s=5.02 Tev
... coincident at the ALICE interaction point) was suffi- ciently small that the chance of two hadronic interactions occurring together, so-called pileup events, was ...layers of which form the silicon ... See full document
13
Nuclear effects on the transverse momentum spectra of charged particles in pPb collisions at root s(NN)=5.02 TeV
... Proton–nucleus collisions have already been used to assess the impact of cold nuclear matter on jet production at the ...and pseudorapidity distributions of dijets have been ... See full document
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D-meson Production In P-pb Collisions At Root S-nn=5.02 Tev And In Pp Collisions At Root S=7 Tev
... information. In addition to the initial-state effects discussed above, also final-state effects may be responsible for a modification of heavy-flavor hadron yields and momentum ...presence of ... See full document
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Lambda(+)(c) production in pp collisions at root s=7 TeV and in p-Pb collisions at root s(NN)=5.02 TeV
... intepretation of the results in nucleus-nucleus collisions, the measurement in proton-nucleus collisions is also ...crucial. In such a system cold-nuclear-matter (CNM) ef- fects ... See full document
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Charged-particle Nuclear Modification Factors In Pbpb And Ppb Collisions At Root S(nn)=5.02 Tev
... features of the QCD confinement cross-over phase transition: suppression of quark and gluon degrees of freedom, and the emergence of chromomagnetic ...central collisions, the model ... See full document
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One-dimensional charged kaon femtoscopy in p-Pb collisions at root s(NN)=5.02 TeV
... Pb-Pb collisions at √ s = 7 TeV [ 13 ] and √ s NN = ...2.76 TeV [ 14 ], ...generated in the Gribov-Regge multiple scattering ...treatment of nonlinear ... See full document
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Measurement of pseudorapidity distributions of charged particles in proton-proton collisions at root s=8 TeV by the CMS and TOTEM experiments
... included in the ...% of the inclusive, NSD-enhanced and SD-enhanced samples, ...effect of removing these events is evaluated in a MC study, which yields over- all correction factors of ... See full document
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J/psi production as a function of charged-particle pseudorapidity density in p-Pb collisions at root s(NN)=5.02 TeV
... B. Paul 113 , H. Pei 7 , T. Peitzmann 53 , X. Peng 7 , L.G. Pereira 63 , H. Pereira Da Costa 65 , D. Peresunko 83 , 76 , E. Perez Lezama 60 , V. Peskov 60 , Y. Pestov 5 , V. Petráˇcek 38 , V. Petrov 114 , M. ... See full document
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Pseudorapidity Dependence Of The Anisotropic Flow Of Charged Particles In Pb-pb Collisions At Root S(nn)=2.76 Tev
... s NN = 2 . 76 TeV using the ALICE ...-range at the LHC, − 3 . 5 < η < 5 . 0, in nine centrality bins covering 0 to 80% of the total inelastic cross ...shape ... See full document
14
Pseudorapidity distribution of charged hadrons in proton-proton collisions at root s=13TeV
... (pp) collisions delivered by the CERN LHC at a center-of-mass energy of 13 TeV in June ...recorded at zero magnetic field during a special low-intensity beam configura- tion ... See full document
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Pseudorapidity distributions of charged hadrons in proton-lead collisions at $\sqrt{s_{_\mathrm{NN}}} =$ 5.02 and 8.16 TeV
... colleagues in the CERN accelerator departments for the excellent perfor- mance of the LHC and thank the technical and administrative staffs at CERN and at other CMS institutes for their ... See full document
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