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
Loading Data...
Please try again later, or email info@hepdata.net if this error persists.
This table is too large to load automatically.
The table size is MB, which is greater than our threshold of MB.
Loading Data...
Please try again later, or email info@hepdata.net if this error persists.
Your question will be emailed to those involved with the submission. Please mention the relevant table.
Please log in to HEPData to send a question.