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[PDF] Top 20 One-dimensional charged kaon femtoscopy in p-Pb collisions at root s(NN)=5.02 TeV

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One-dimensional charged kaon femtoscopy in p-Pb collisions at root s(NN)=5.02 TeV

One-dimensional charged kaon femtoscopy in p-Pb collisions at root s(NN)=5.02 TeV

... Development in the South (COMSATS), Pakistan; Pontificia Universidad Católica del Perú, Peru; Ministry of Science and Higher Education and National Science Centre, Poland; Korea Institute of Science and Technology ... See full document

16

Multiplicity dependence of pion, kaon, proton and lambda production in p-Pb collisions at root s(NN)=5.02 TeV

Multiplicity dependence of pion, kaon, proton and lambda production in p-Pb collisions at root s(NN)=5.02 TeV

... (pA) collisions are intermediate between pro- ton–proton (pp) and nucleus–nucleus (AA) collisions in terms of system size and number of produced ...production in pp, pA, and AA reactions has ... See full document

15

J/psi production as a function of charged-particle pseudorapidity density in p-Pb collisions at root s(NN)=5.02 TeV

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

15

Measurement of D0, D+, D*+ and Ds+ production in Pb-Pb collisions at root s(NN)=5:02 TeV

Measurement of D0, D+, D*+ and Ds+ production in Pb-Pb collisions at root s(NN)=5:02 TeV

... the one used in previous analyses [ 25 , 39 ] and is mainly based on the separation between primary and secondary vertex, the displacement of the tracks from the primary vertex and the pointing of the ... See full document

36

Transverse momentum dependence of inclusive primary charged-particle production in p–Pb collisions at root S-NN=5.02 TeV

Transverse momentum dependence of inclusive primary charged-particle production in p–Pb collisions at root S-NN=5.02 TeV

... . Turrisi 102 , T. S. Tveter 21 , K. Ullaland 17 , A. Uras 122 , G. L. Usai 23 , M. Vajzer 77 , M. Vala 54 ,61 , L. Valencia Palomo 64 , S. Vallero 87 , P. Vande Vyvre 34 , J. Van Der Maarel 52 , J. ... See full document

11

Centrality Dependence Of Charged Jet Production In P-pb Collisions At Root(nn)-n-s=5.02 Tev

Centrality Dependence Of Charged Jet Production In P-pb Collisions At Root(nn)-n-s=5.02 Tev

... J. de Cuveland 42 , A. De Falco 24 , D. De Gruttola 30 , 12 , N. De Marco 110 , S. De Pasquale 30 , A. Deisting 94 , 97 , A. Deloff 77 , E. Dénes 136 , a , C. Deplano 82 , P. Dhankher 47 , D. Di Bari 32 , ... See full document

16

Anisotropic Flow Of Charged Particles In Pb-pb Collisions At Root S-nn=5.02 Tev

Anisotropic Flow Of Charged Particles In Pb-pb Collisions At Root S-nn=5.02 Tev

... D. Mcdonald, 122 F. Meddi, 23 Y. Melikyan, 75 A. Menchaca-Rocha, 64 E. Meninno, 30 J. Mercado Pérez, 94 M. Meres, 38 Y. Miake, 128 M. M. Mieskolainen, 45 K. Mikhaylov, 66,58 L. Milano, 35,74 J. Milosevic, 22 A. Mischke, ... See full document

13

Energy dependence and fluctuations of anisotropic fow in Pb-Pb collisions at root s(NN)=5:02 and 2:76 TeV

Energy dependence and fluctuations of anisotropic fow in Pb-Pb collisions at root s(NN)=5:02 and 2:76 TeV

... necessary, in wider centrality intervals using the charged particle yield in each 1% centrality bin as ...bias in the average centrality within a large centrality bin, since multiplicity ... See full document

40

Measurement of dijet k(T) in p-Pb collisions at root s(NN)=5.02 TeV

Measurement of dijet k(T) in p-Pb collisions at root s(NN)=5.02 TeV

... the charged energy ...by charged tracks in the EMCal, the EMCal energy scale and the charged particle tracking efficiency and p T ...of p T , jet of the full and associated ... See full document

12

Forward-central Two-particle Correlations In P-pb Collisions At Root S(nn)=5.02 Tev

Forward-central Two-particle Correlations In P-pb Collisions At Root S(nn)=5.02 Tev

... from one event with the associated particles from other events within the same event multiplicity class and 1 cm-wide z vtx ...unity in the  η region of maximal pair ...correlations in ... See full document

15

Centrality dependence of particle production in p-Pb collisions at root s(NN)=5.02 TeV

Centrality dependence of particle production in p-Pb collisions at root s(NN)=5.02 TeV

... However, one can study the correlation of two or more observables out of which at least one is expected to scale linearly with N coll ...multiplicity at midrapidity proportional to the number ... See full document

29

Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at root s(NN)=5.02 TeV

Centrality dependence of the pseudorapidity density distribution for charged particles in Pb-Pb collisions at root s(NN)=5.02 TeV

... the charged-particle pseudorapidity den- sity at mid-rapidity ( | η | < 2) is obtained from a tracklet analysis using the two layers of the ...ations in the number of strange particles or ... See full document

12

Centrality Dependence Of The Charged-particle Multiplicity Density At Midrapidity In Pb-pb Collisions At Root(nn)-n-s=5.02 Tev

Centrality Dependence Of The Charged-particle Multiplicity Density At Midrapidity In Pb-pb Collisions At Root(nn)-n-s=5.02 Tev

... nucleon-nucleon collisions, and f ∼ ...contribution at high multiplicity. In the Monte Carlo Glauber calculation, the nuclear density for 208 Pb is modeled by a Woods-Saxon distribution for a ... See full document

13

Measurement of charged jet production cross sections and nuclear modification in p-Pb collisions at root s(NN)=5.02 TeV

Measurement of charged jet production cross sections and nuclear modification in p-Pb collisions at root s(NN)=5.02 TeV

... sections in pPb collisions ats NN = 5 .... 02 TeV measured with the ALICE detector at the LHC are ...reconstructed in the central rapidity ... See full document

15

Measurement of electrons from beauty-hadron decays in p-Pb collisions at root(NN)-N-S=5.02 TeV and Pb-Pb collisions at. root(NN)-N-S=2.76 TeV

Measurement of electrons from beauty-hadron decays in p-Pb collisions at root(NN)-N-S=5.02 TeV and Pb-Pb collisions at. root(NN)-N-S=2.76 TeV

... (hits in both SPD layers) does not depend strongly on the particle ...Thus, charged tracks could be used as a represen- tative sample with respect to the geometric effects, such as inactive areas of the ... See full document

41

W And Z Boson Production In P-pb Collisions At Tev Root S(nn)=5.02 Tev

W And Z Boson Production In P-pb Collisions At Tev Root S(nn)=5.02 Tev

... shown in figure 2 ...uncertainties. In particular, six additional templates were produced, corresponding to the upper and lower limits of the calculations obtained by i) varying the factorisation and ... See full document

28

Two-pion femtoscopy in p-Pb collisions at root(NN)-N-S=5.02 TeV

Two-pion femtoscopy in p-Pb collisions at root(NN)-N-S=5.02 TeV

... observed in data, which is another argument for their nonfemtoscopic ...differences in the magnitude and shape of these structures when compared to those observed in data are seen for AMPT , HIJING , ... See full document

19

Lambda(+)(c) production in pp collisions at root s=7 TeV and in p-Pb collisions at root s(NN)=5.02 TeV

Lambda(+)(c) production in pp collisions at root s=7 TeV and in p-Pb collisions at root s(NN)=5.02 TeV

... azimuth in the pseudorapidity intervals ...detectors. At least one hit in either of the two scintillator arrays of the V0, or at least one hit in the SPD (pseudorapidity ... See full document

49

Charged-particle pseudorapidity density at mid-rapidity in p-Pb collisions at root S-NN=8.16 TeV

Charged-particle pseudorapidity density at mid-rapidity in p-Pb collisions at root S-NN=8.16 TeV

... the one employed ats NN = 5.02 TeV [ 31 , 34 ...acceptance in the laboratory system depends on the position of the primary interaction vertex along the beamline, z ...hits in ... See full document

18

Multiplicity Dependence Of Charged Pion, Kaon, And (anti)proton Production At Large Transverse Momentum In P-pb Collisions Root S-nn=5.02 Tev

Multiplicity Dependence Of Charged Pion, Kaon, And (anti)proton Production At Large Transverse Momentum In P-pb Collisions Root S-nn=5.02 Tev

... of In- dia; Instituto Nazionale di Fisica Nucleare (INFN) and Centro Fermi – Museo Storico della Fisica e Centro Studi e Ricerche “Enrico Fermi”, Italy; Japan Society for the Promotion of Science (JSPS) KAKENHI ... See full document

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