Measured differential yield of charged hadrons as a function oftransverse momentum for the pseudorapidity range -2.4 to +2.4 for centre-of-mass energy 7000 GeV. Errors are statistical and systematic added in quadrature.

Reconstructed differential charged hadron yields as a function of pseudorapidity averaged over the three methods methodsat a centre-of-mass energy of 7000 GeV.Errors shown are systematic (4 pct).Systematic errors are less than 0.5 pct of the values.

7 TeV Particle density vs. Delta(phi) with leading particle pT > 1 GeV.

7 TeV Particle density vs. Delta(phi) with leading particle pT > 2 GeV.

7 TeV Particle density vs. Delta(phi) with leading particle pT > 3 GeV.

900 GeV Transverse region Particle density vs. leading particle pT.

7 TeV Transverse region Particle density vs. leading particle pT.

900 GeV Transverse region scalar pT sum density vs. leading particle pT.

7 TeV Transverse region scalar pT sum density vs. leading particle pT.

Fully corrected average charged particle scalar PT Sum per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 0.9 TeV.

Fully corrected average charged particle scalar PT Sum per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 7 TeV.

Ratio of the fully corrected average charged particle scalar PT Sum at 7 TeV to that at 0.9 TeV.

Normalized multiplicity distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 0.9 TeV with the leading track-jet transverse momentum > 3 GeV.

Normalized multiplicity distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 7 TeV with the leading track-jet transverse momentum > 3 GeV.

Normalized multiplicity distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 7 TeV with the leading track-jet transverse momentum > 20 GeV.

Normalized scalar PT Sum distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 0.9 TeV with the leading track-jet transverse momentum > 3 GeV.

Normalized scalar PT Sum distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 7 TeV with the leading track-jet transverse momentum > 3 GeV.

Normalized scalar PT Sum distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 7 TeV with the leading track-jet transverse momentum > 20 GeV.

PT distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 0.9 TeV with the leading track-jet transverse momentum > 3 GeV.

PT distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 7 TeV with the leading track-jet transverse momentum > 3 GeV.

PT distribution of charged particles produced in proton-proton collisions at a center-of-mass energy of 7 TeV with the leading track-jet transverse momentum > 20 GeV.

The inclusive charged particle invariant differential cross section, as a function of XT and scaled by sqrt(s)*4.9, at 7 TeV for |eta|<1.

The interpolated invariant charged particle differential cross section at 2.76 GeV for |eta|<1.

Charged particle fragmentation function in the jet-Pt range 80 TO 110 GeV.

Charged particle fragmentation function in the jet-Pt range 110 TO 160 GeV.

Charged particle fragmentation function in the jet-Pt range 160 TO 210 GeV.

Charged particle fragmentation function in the jet-Pt range 210 TO 260 GeV.

Charged particle fragmentation function in the jet-Pt range 260 TO 310 GeV.

Charged particle fragmentation function in the jet-Pt range 310 TO 400 GeV.

Charged particle fragmentation function in the jet-Pt range 400 TO 500 GeV.

Charged particle Rho distribution in the jet-Pt range 25 TO 40 GeV.

Charged particle Rho distribution in the jet-Pt range 40 TO 60 GeV.

Charged particle Rho distribution in the jet-Pt range 60 TO 80 GeV.

Charged particle Rho distribution in the jet-Pt range 80 TO 110 GeV.

Charged particle Rho distribution in the jet-Pt range 110 TO 160 GeV.

Charged particle Rho distribution in the jet-Pt range 160 TO 210 GeV.

Charged particle Rho distribution in the jet-Pt range 210 TO 260 GeV.

Charged particle Rho distribution in the jet-Pt range 260 TO 310 GeV.

Charged particle Rho distribution in the jet-Pt range 310 TO 400 GeV.

Charged particle Rho distribution in the jet-Pt range 400 TO 500 GeV.

Charged particle ptRel distribution in the jet-Pt range 25 TO 40 GeV.

Charged particle ptRel distribution in the jet-Pt range 40 TO 60 GeV.

Charged particle ptRel distribution in the jet-Pt range 60 TO 80 GeV.

Charged particle ptRel distribution in the jet-Pt range 80 TO 110 GeV.

Charged particle ptRel distribution in the jet-Pt range 110 TO 160 GeV.

Charged particle ptRel distribution in the jet-Pt range 160 TO 210 GeV.

Charged particle ptRel distribution in the jet-Pt range 210 TO 260 GeV.

Charged particle ptRel distribution in the jet-Pt range 260 TO 310 GeV.

Charged particle ptRel distribution in the jet-Pt range 310 TO 400 GeV.

Charged particle ptRel distribution in the jet-Pt range 400 TO 500 GeV.

Distribution of the heavy particle Mass estimated from the Tile Calorimeter data plus the simulated background and model estimates for three gluino masses. A cut of BETA < 1 is imposed.;.

Distribution of the heavy particle Mass estimated from the Pixel detector data plus the data driven background and model estimates for two gluino masses.;.

Distribution of the heavy particle Mass estimated from the Tile Calorimeter data plus the data driven background and model estimates for two gluino masses.;.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 1.5 at a centre-of-mass energy of 900 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 2.0 at a centre-of-mass energy of 900 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 2.4 at a centre-of-mass energy of 900 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 0.5 at a centre-of-mass energy of 2360 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 1.0 at a centre-of-mass energy of 2360 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 1.5 at a centre-of-mass energy of 2360 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 2.0 at a centre-of-mass energy of 2360 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 2.4 at a centre-of-mass energy of 2360 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 0.5 at a centre-of-mass energy of 7000 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 1.0 at a centre-of-mass energy of 7000 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 1.5 at a centre-of-mass energy of 7000 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 2.0 at a centre-of-mass energy of 7000 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 2.4 at a centre-of-mass energy of 7000 GeV.

Normalised moments C_Q at a centre-of-mass energy of 0.9 TeV.

Normalised moments C_Q at a centre-of-mass energy of 2.36 TeV.

Normalised moments C_Q at a centre-of-mass energy of 7.0 TeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 2.4 and PT > 500 MeV at a centre-of-mass energy of 900 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 2.4 and PT > 500 MeV at a centre-of-mass energy of 2360 GeV.

Fully corrected charged hadron multiplicity spectrum for |pseudorapidity| < 2.4 and PT > 500 MeV at a centre-of-mass energy of 7000 GeV.

Mean transverse momentum for |pseudorapidity| < 2.4 at a centre-of-mass energy of 900 GeV.

Mean transverse momentum for |pseudorapidity| < 2.4 at a centre-of-mass energy of 2360 GeV.

Mean transverse momentum for |pseudorapidity| < 2.4 at a centre-of-mass energy of 7000 GeV.

The charged hadron multiplicity distributions in KNO form for |pseudorapidity| < 0.5 at a centre-of-mass energy of 900 GeV.

The charged hadron multiplicity distributions in KNO form for |pseudorapidity| < 2.4 at a centre-of-mass energy of 900 GeV.

The charged hadron multiplicity distributions in KNO form for |pseudorapidity| < 0.5 at a centre-of-mass energy of 7000 GeV.

The charged hadron multiplicity distributions in KNO form for |pseudorapidity| < 2.4 at a centre-of-mass energy of 7000 GeV.

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 1.0 $<p_{T}<$ 2.0 $GeV/c$ and $N_{offline}^{trk}<$ 35 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 2.0 $<p_{T}<$ 3.0 $GeV/c$ and $N_{offline}^{trk}<$ 35 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 2.0 $<p_{T}<$ 3.0 $GeV/c$ and $N_{offline}^{trk}<$ 35 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 3.0 $<p_{T}<$ 4.0 $GeV/c$ and $N_{offline}^{trk}<$ 35 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 3.0 $<p_{T}<$ 4.0 $GeV/c$ and $N_{offline}^{trk}<$ 35 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 0.1 $<p_{T}<$ 1.0 $GeV/c$ and 35 $<N_{offline}^{trk}<$ 80 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 0.1 $<p_{T}<$ 1.0 $GeV/c$ and 35 $<N_{offline}^{trk}<$ 90 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 1.0 $<p_{T}<$ 2.0 $GeV/c$ and 35 $<N_{offline}^{trk}<$ 80 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 1.0 $<p_{T}<$ 2.0 $GeV/c$ and 35 $<N_{offline}^{trk}<$ 90 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 2.0 $<p_{T}<$ 3.0 $GeV/c$ and 35 $<N_{offline}^{trk}<$ 80 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 2.0 $<p_{T}<$ 3.0 $GeV/c$ and 35 $<N_{offline}^{trk}<$ 90 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 3.0 $<p_{T}<$ 4.0 $GeV/c$ and 35 $<N_{offline}^{trk}<$ 80 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 3.0 $<p_{T}<$ 4.0 $GeV/c$ and 35 $<N_{offline}^{trk}<$ 90 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 0.1 $<p_{T}<$ 1.0 $GeV/c$ and 80 $<N_{offline}^{trk}<$ 105 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 0.1 $<p_{T}<$ 1.0 $GeV/c$ and 90 $<N_{offline}^{trk}<$ 105 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 1.0 $<p_{T}<$ 2.0 $GeV/c$ and 80 $<N_{offline}^{trk}<$ 105 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 1.0 $<p_{T}<$ 2.0 $GeV/c$ and 90 $<N_{offline}^{trk}<$ 105 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 2.0 $<p_{T}<$ 3.0 $GeV/c$ and 80 $<N_{offline}^{trk}<$ 105 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 2.0 $<p_{T}<$ 3.0 $GeV/c$ and 90 $<N_{offline}^{trk}<$ 105 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 3.0 $<p_{T}<$ 4.0 $GeV/c$ and 80 $<N_{offline}^{trk}<$ 105 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 3.0 $<p_{T}<$ 4.0 $GeV/c$ and 90 $<N_{offline}^{trk}<$ 105 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 0.1 $<p_{T}<$ 1.0 $GeV/c$ and $N_{offline}^{trk}>$ 105 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 0.1 $<p_{T}<$ 1.0 $GeV/c$ and $N_{offline}^{trk}>$ 110 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 1.0 $<p_{T}<$ 2.0 $GeV/c$ and $N_{offline}^{trk}>$ 105 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 1.0 $<p_{T}<$ 2.0 $GeV/c$ and $N_{offline}^{trk}>$ 110 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 2.0 $<p_{T}<$ 3.0 $GeV/c$ and $N_{offline}^{trk}>$ 105 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 2.0 $<p_{T}<$ 3.0 $GeV/c$ and $N_{offline}^{trk}>$ 110 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 3.0 $<p_{T}<$ 4.0 $GeV/c$ and $N_{offline}^{trk}>$ 105 bins for pp data at $\sqrt =$ 13 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Correlated yield obtained with the ZYAM procedure as a function of $|\Delta\Phi|$, averaged over 2 $<|\Delta\eta|<$ 4 in for 3.0 $<p_{T}<$ 4.0 $GeV/c$ and $N_{offline}^{trk}>$ 110 bins for pp data at $\sqrt =$ 7 $TeV$. The $p_{T}$ selection applies to both particles in the pair. Only statistical uncertainties are given. The subtracted ZYAM constant is given ($C_{ZYAM}$).

Associated yield for the near side of the correlation function averaged over 2 $<|\Delta\eta|<$ 4 and integrated over the region $|\Delta\Phi| < \Delta\Phi_{ZYAM}$ for pp data at $\sqrt{s} =$ 13 $TeV$. The associated yield as a function of $p_{T}$ for events with $N^{offline}_{trk} \geq$ 105. The $p_{T}$ value for each $p_{T}$ bin is the average $p_{T}$ value.

Associated yield for the near side of the correlation function averaged over 2 $<|\Delta\eta|<$ 4 for pp data at $\sqrt{s} =$ 7 $TeV$. The associated yield as a function of $p_{T}$ for events with $N^{offline}_{trk} \geq$ 110. The $p_{T}$ value for each $p_{T}$ bin is the average $p_{T}$ value.

Associated yield for the near side of the correlation function averaged over 2 $<|\Delta\eta|<$ 4 and integrated over the region $|\Delta\Phi| < \Delta\Phi_{ZYAM}$ for pp data at $\sqrt{s} =$ 13 $TeV$. The associated yield as a function of $N_{trk}^{offline}$ for events with 1.0 $< p_{T} <$ 2.0 GeV/c. The $N_{trk}^{offline}$ value for each $N_{trk}^{offline}$ bin is the average $N_{trk}^{offline}$ value.

Associated yield for the near side of the correlation function averaged over 2 $<|\Delta\eta|<$ 4 for pp data at $\sqrt{s} =$ 7 $TeV$. The associated yield as a function of $N_{trk}^{offline}$ for events with 1.0 $< p_{T} <$ 2.0 GeV/c. The $N_{trk}^{offline}$ value for each $N_{trk}^{offline}$ bin is the average $N_{trk}^{offline}$ value.

Associated yield for the near side of the correlation function averaged over 2 $<|\Delta\eta|<$ 4 pPb data at $\sqrt{s} =$ 5.02 $TeV$. The associated yield as a function of $N_{trk}^{offline}$ for events with 1.0 $< p_{T} <$ 2.0 GeV/c. The $N_{trk}^{offline}$ value for each $N_{trk}^{offline}$ bin is the average $N_{trk}^{offline}$ value.

Associated yield for the near side of the correlation function averaged over 2 $<|\Delta\eta|<$ 4 PbPb data at $\sqrt{s} =$ 2.76 $TeV$. The associated yield as a function of $N_{trk}^{offline}$ for events with 1.0 $< p_{T} <$ 2.0 GeV/c. The $N_{trk}^{offline}$ value for each $N_{trk}^{offline}$ bin is the average $N_{trk}^{offline}$ value.

The Symmetric cumulant $SC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

The Symmetric cumulant $SC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in pPb collisions at $\sqrt{s_{NN}}$ = 8.16 TeV.

The Symmetric cumulant $SC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in pp collisions at $\sqrt{s}$ = 13.0 TeV.

The Normalized Symmetric cumulant $NSC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. The results are normalized by $\left<(v_2^{\text{sub}})^{2}\right> \, \left<(v_3^{\text{sub}})^{2}\right>$ and $\left<(v_2^{\text{sub}})^{2}\right> \, \left<(v_4^{\text{sub}})^{2}\right>$ from two-particle correlations.

The Normalized Symmetric cumulant $NSC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in pPb collisions at $\sqrt{s_{NN}}$ = 8.16 TeV. The results are normalized by $\left<(v_2^{\text{sub}})^{2}\right> \, \left<(v_3^{\text{sub}})^{2}\right>$ and $\left<(v_2^{\text{sub}})^{2}\right> \, \left<(v_4^{\text{sub}})^{2}\right>$ from two-particle correlations.

The Normalized Symmetric cumulant $NSC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in pp collisions at $\sqrt{s}$ = 13.0 TeV. The results are normalized by $\left<(v_2^{\text{sub}})^{2}\right> \, \left<(v_3^{\text{sub}})^{2}\right>$ and $\left<(v_2^{\text{sub}})^{2}\right> \, \left<(v_4^{\text{sub}})^{2}\right>$ from two-particle correlations.