Table 1
Data from Figure 1 (top left)
10.17182/hepdata.83969.v1/t1
The symmetric cumulant $sc_{2,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 1 (top left)
10.17182/hepdata.83969.v1/t1
The symmetric cumulant $sc_{2,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 1 (top right)
10.17182/hepdata.83969.v1/t2
The symmetric cumulant $sc_{2\,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 1 (middle left)
10.17182/hepdata.83969.v1/t3
The symmetric cumulant $sc_{2\,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 1 (middle right)
10.17182/hepdata.83969.v1/t4
The symmetric cumulant $sc_{2\,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 1 (bottom left)
10.17182/hepdata.83969.v1/t5
The symmetric cumulant $sc_{2\,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 1 (bottom right)
10.17182/hepdata.83969.v1/t6
The symmetric cumulant $sc_{2\,4}\{4\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 2 (top left)
10.17182/hepdata.83969.v1/t7
The symmetric cumulant $sc_{2\,4}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 2 (top right)
10.17182/hepdata.83969.v1/t8
The symmetric cumulant $sc_{2\,4}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 2 (middle left)
10.17182/hepdata.83969.v1/t9
The symmetric cumulant $sc_{2\,4}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 2 (middle right)
10.17182/hepdata.83969.v1/t10
The symmetric cumulant $sc_{2\,4}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 2 (bottom left)
10.17182/hepdata.83969.v1/t11
The symmetric cumulant $sc_{2\,4}\{4\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 2 (bottom right)
10.17182/hepdata.83969.v1/t12
The symmetric cumulant $sc_{2\,4}\{4\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 3 (top left)
10.17182/hepdata.83969.v1/t13
The asymmetric cumulant $ac_{2}\{3\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 3 (top right)
10.17182/hepdata.83969.v1/t14
The asymmetric cumulant $ac_{2}\{3\}$results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 3 (middle left)
10.17182/hepdata.83969.v1/t15
The asymmetric cumulant $ac_{2}\{3\}$results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 3 (middle right)
10.17182/hepdata.83969.v1/t16
The asymmetric cumulant $ac_{2}\{3\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 3 (bottom left)
10.17182/hepdata.83969.v1/t17
The asymmetric cumulant $ac_{2}\{3\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 3 (bottom right)
10.17182/hepdata.83969.v1/t18
The asymmetric cumulant $ac_{2}\{3\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 5 (top left)
10.17182/hepdata.83969.v1/t19
The normalized symmetric cumulant $nsc_{2\,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 5 (top middle)
10.17182/hepdata.83969.v1/t20
The normalized symmetric cumulant $nsc_{2\,4}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 5 (top right)
10.17182/hepdata.83969.v1/t21
The normalized asymmetric cumulant $nac_{2}\{3\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 5 (bottom left)
10.17182/hepdata.83969.v1/t22
The normalized symmetric cumulant $nsc_{2\,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 5 (bottom middle)
10.17182/hepdata.83969.v1/t23
The normalized symmetric cumulant $nsc_{2\,4}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 5 (bottom right)
10.17182/hepdata.83969.v1/t24
The normalized asymmetric cumulant $nac_{2}\{3\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 5 (top left)
10.17182/hepdata.83969.v1/t25
The normalized symmetric cumulant $nsc_{2\,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 5 (top middle)
10.17182/hepdata.83969.v1/t26
The normalized symmetric cumulant $nsc_{2\,4}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 5 (top right)
10.17182/hepdata.83969.v1/t27
The normalized asymmetric cumulant $nac_{2}\{3\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 5 (bottom left)
10.17182/hepdata.83969.v1/t28
The normalized symmetric cumulant $nsc_{2\,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 5 (bottom middle)
10.17182/hepdata.83969.v1/t29
The normalized symmetric cumulant $nsc_{2\,4}\{4\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 5 (bottom right)
10.17182/hepdata.83969.v1/t30
The normalized asymmetric cumulant $nac_{2}\{3\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 5 (top left)
10.17182/hepdata.83969.v1/t31
The normalized symmetric cumulant $nsc_{2\,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 5 (top middle)
10.17182/hepdata.83969.v1/t32
The normalized symmetric cumulant $nsc_{2\,4}\{4\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 5 (top right)
10.17182/hepdata.83969.v1/t33
The normalized asymmetric cumulant $nac_{2}\{3\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 5 (bottom left)
10.17182/hepdata.83969.v1/t34
The normalized symmetric cumulant $nsc_{2\,3}\{4\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 5 (bottom middle)
10.17182/hepdata.83969.v1/t35
The normalized symmetric cumulant $nsc_{2\,4}\{4\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 5 (bottom right)
10.17182/hepdata.83969.v1/t36
The normalized asymmetric cumulant $nac_{2}\{3\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 7 (top left)
10.17182/hepdata.83969.v1/t37
The $v_{2}\{2\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 7 (top middle)
10.17182/hepdata.83969.v1/t38
The $v_{3}\{2\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 7 (top right)
10.17182/hepdata.83969.v1/t39
The $v_{4}\{2\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data from Figure 7 (middle left)
10.17182/hepdata.83969.v1/t40
The $v_{2}\{2\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 7 (middle middle)
10.17182/hepdata.83969.v1/t41
The $v_{3}\{2\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 7 (middle right)
10.17182/hepdata.83969.v1/t42
The $v_{4}\{2\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data from Figure 7 (bottom left)
10.17182/hepdata.83969.v1/t43
The $v_{2}\{2\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 7 (bottom middle)
10.17182/hepdata.83969.v1/t44
The $v_{3}\{2\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 7 (bottom right)
10.17182/hepdata.83969.v1/t45
The $v_{4}\{2\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data similar to Figure 7 (top left) but for higher pT
10.17182/hepdata.83969.v1/t46
The $v_{2}\{2\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data similar to Figure 7 (top middle) but for higher pT
10.17182/hepdata.83969.v1/t47
The $v_{3}\{2\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data similar to Figure 7 (top right) but for higher pT
10.17182/hepdata.83969.v1/t48
The $v_{4}\{2\}$ results as a function of multiplicity ($N_{ch}$) in pp collisions at $\sqrt{s_{NN}}$ = 13 TeV
Data similar to Figure 7 (middle left) but for higher pT
10.17182/hepdata.83969.v1/t49
The $v_{2}\{2\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data similar to Figure 7 (middle middle) but for higher pT
10.17182/hepdata.83969.v1/t50
The $v_{3}\{2\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data similar to Figure 7 (middle right) but for higher pT
10.17182/hepdata.83969.v1/t51
The $v_{4}\{2\}$ results as a function of multiplicity ($N_{ch}$) in pPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV
Data similar to Figure 7 (bottom left) but for higher pT
10.17182/hepdata.83969.v1/t52
The $v_{2}\{2\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data similar to Figure 7 (bottom middle) but for higher pT
10.17182/hepdata.83969.v1/t53
The $v_{3}\{2\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data similar to Figure 7 (bottom right) but for higher pT
10.17182/hepdata.83969.v1/t54
The $v_{4}\{2\}$ results as a function of multiplicity ($N_{ch}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV
Data from Figure 8 (left)
10.17182/hepdata.83969.v1/t55
The symmetric cumulant $ac_{2}\{3\}$ in Pb+Pb from different methods
Data from Figure 8 (right)
10.17182/hepdata.83969.v1/t56
The symmetric cumulant $ac_{2}\{3\}$ in Pb+Pb from different methods
Data from Figure 9 (left)
10.17182/hepdata.83969.v1/t57
The symmetric cumulant $ac_{2}\{3\}$ in p+Pb from different methods
Data from Figure 9 (right)
10.17182/hepdata.83969.v1/t58
The symmetric cumulant $ac_{2}\{3\}$ in p+Pb from different methods
Data from Figure 10 (left)
10.17182/hepdata.83969.v1/t59
The symmetric cumulant $ac_{2}\{3\}$ in pp from different methods
Data from Figure 10 (right)
10.17182/hepdata.83969.v1/t60
The symmetric cumulant $ac_{2}\{3\}$ in pp from different methods
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