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[PDF] Top 20 Charged-particle production as a function of multiplicity and transverse spherocity in pp collisions at root s=5.02 and 13 TeV

Has 10000 "Charged-particle production as a function of multiplicity and transverse spherocity in pp collisions at root s=5.02 and 13 TeV" found on our website. Below are the top 20 most common "Charged-particle production as a function of multiplicity and transverse spherocity in pp collisions at root s=5.02 and 13 TeV".

Charged-particle production as a function of multiplicity and transverse spherocity in pp collisions at root s=5.02 and 13 TeV

Charged-particle production as a function of multiplicity and transverse spherocity in pp collisions at root s=5.02 and 13 TeV

... Science and Education, Croatia; Centro de Aplicaciones Tecnológ- icas y Desarrollo Nuclear (CEADEN), Cubaenergía, Cuba; Ministry of Education, Youth and Sports of the Czech Republic, Czech ... See full document

23

D-meson Production In P-pb Collisions At Root S-nn=5.02 Tev And In Pp Collisions At Root S=7 Tev

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

32

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

... 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

49

Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at root s=13 TeV

Dielectron and heavy-quark production in inelastic and high-multiplicity proton-proton collisions at root s=13 TeV

... this, pp events are generated with the Monash 2013 tune of Pythia 8 [ 52 ] for light-hadron decays and the Perugia 2011 tune of Pythia ...] and the resulting particles are prop- agated ... 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

Centrality and pseudorapidity dependence of the charged-particle multiplicity density in Xe-Xe collisions at root s(NN)=5.44 TeV

Centrality and pseudorapidity dependence of the charged-particle multiplicity density in Xe-Xe collisions at root s(NN)=5.44 TeV

... analysis at mid-rapidity the relative systematic uncertainty on the measurement of the charged-particle multiplic- ity in peripheral (central) events arises from the following sources: ... See full document

15

Measurement of charged pion, kaon, and proton production in proton-proton collisions at root s=13 TeV

Measurement of charged pion, kaon, and proton production in proton-proton collisions at root s=13 TeV

... where pp collisions occur (beam spot) is measured from the distribution of reconstructed interaction ...narrow in the plane transverse to the beam direction (with a width of ... See full document

25

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

... U. Tabassam 16 , J. Takahashi 121 , G.J. Tambave 18 , N. Tanaka 128 , M.A. Tangaro 33 , M. Tarhini 51 , M. Tariq 19 , M.G. Tarzila 78 , A. Tauro 36 , G. Tejeda Muñoz 2 , A. Telesca 36 , K. Terasaki 127 , C. Terrevoli 30 ... See full document

17

Study of the inclusive production of charged pions, kaons, and protons in pp collisions at root s=0.9, 2.76, and 7 TeV

Study of the inclusive production of charged pions, kaons, and protons in pp collisions at root s=0.9, 2.76, and 7 TeV

... the particle-specific momentum ranges for the following procedures: counting the yields (Count); using a particle species in the fits (Fit, paragraphs a and b in ...losses in the ... See full document

37

Study of high-p(T) charged particle suppression in PbPb compared to pp collisions at root s(NN)=2.76 TeV

Study of high-p(T) charged particle suppression in PbPb compared to pp collisions at root s(NN)=2.76 TeV

... description of the CMS detector can be found in ...feature of the CMS apparatus is a superconducting solenoid of 6 m internal diameter, providing an axial magnetic field of ...Immersed ... See full document

22

Measurement of long-range near-side two-particle angular correlations in pp collisions at root s=13 TeV

Measurement of long-range near-side two-particle angular correlations in pp collisions at root s=13 TeV

... studies in Ref. [29] , the total systematic uncertainty of the tracking efficiency is ...uncertainty of the asso- ciated ...z and d T =σ d T between 2 and ...0.0006 in absolute ... See full document

20

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

... 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 ... See full document

36

Charged-particle nuclear modification factors in XeXe collisions at root S-NN=5.44 TeV

Charged-particle nuclear modification factors in XeXe collisions at root S-NN=5.44 TeV

... some charged particles, notably the strange baryons, are more likely to decay into secondary particles which then contaminate the ...dependence of the total tracking correction, because different MC event ... See full document

43

Charged-particle multiplicities in proton-proton collisions at root s=0.9 to 8 TeV

Charged-particle multiplicities in proton-proton collisions at root s=0.9 to 8 TeV

... cm in z. This was confirmed by simulating events, where two Monte Carlo pp collisions were superimposed, demonstrating that only 5% of the events passing the selec- tion had extra ... See full document

40

Measurement of charged particle spectra in minimum-bias events from proton-proton collisions at root s =13 TeV

Measurement of charged particle spectra in minimum-bias events from proton-proton collisions at root s =13 TeV

... tracking and event selection effi- ciencies, as well as for detector resolution ...primary charged par- ticles, which are either directly produced in pp collisions or result from decays ... See full document

29

Production of charged pions, kaons and protons at large transverse momenta in Pp and Pb-pb collisions at √snn=2.76 Tev

Production of charged pions, kaons and protons at large transverse momenta in Pp and Pb-pb collisions at √snn=2.76 Tev

... inclusive charged particle p T spectrum as has been seen at RHIC [11,12] and over an extended p T range, up to 100 GeV / c, at the LHC [13,14] ...by particle identification (PID) ... See full document

13

Correlations between jets and charged particles in PbPb and pp collisions at root s(NN)=2.76 TeV

Correlations between jets and charged particles in PbPb and pp collisions at root s(NN)=2.76 TeV

... evaluation of the jet and track reconstruction performance, in particular for determining the tracking efficiency as well as the jet energy response and ...response. In order to account ... See full document

40

Multiplicity dependence of light-flavor hadron production in pp collisions at root s=7 TeV

Multiplicity dependence of light-flavor hadron production in pp collisions at root s=7 TeV

... γ S = 1, and the chemical potentials associated to baryon and electric charge quantum numbers are set to ...as in Ref. [ 6 ], following recent results from lattice QCD calculations and ... See full document

31

Charged-particle Nuclear Modification Factors In Pbpb And Ppb Collisions At Root S(nn)=5.02 Tev

Charged-particle Nuclear Modification Factors In Pbpb And Ppb Collisions At Root S(nn)=5.02 Tev

... programme and the Euro- pean Research Council and EPLANET (European Union); the Leventis Foundation; the ...Ministry of Education, Youth and Sports (MEYS) of the Czech Republic; the ... See full document

46

Measurement of charged jet cross section in pp collisions at root s=5.02 TeV

Measurement of charged jet cross section in pp collisions at root s=5.02 TeV

... section of jets reconstructed from charged particles is measured in the transverse momentum range of 5 < p T < 100 GeV=c in pp collisions at the ... See full document

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