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CMS-PAS-HIN-16-022
Correlations of azimuthal anisotropy harmonics in pp, pPb, and PbPb collisions at the LHC
Abstract: The first measurements of anisotropy harmonics (vn, n= 2-4) in pPb collisions at sNN= 8.16 TeV is presented. In addition, measurements of event-by-event correlations of different vn in pp at s= 13 TeV, pPb at sNN= 5.02 and 8.16 TeV and PbPb at sNN= 5.02 TeV collision systems at the LHC are explored. New results of the vn harmonics in 8.16 TeV pPb collisions are extracted via long-range (|Δη|> 2) two-particle correlations as a function of event multiplicity. The current measurement is reaching a very-high-multiplicity region beyond that achieved in 5.02 TeV pPb data collected in 2013. Event-by-event correlations among v2, v3 and v4 harmonics are measured using the four-particle symmetric cumulant method in pp and pPb, and compared to the large system of PbPb collisions. For high-multiplicity (more than 100 tracks) pp and pPb events, the v2 harmonic is found to have a negative correlation with the v3 harmonic, while the v2 and v4 harmonics are positively correlated. Normalized by the two-particle vn harmonics, the correlation coefficients of v2 and v3 harmonics are quantitatively similar for pPb and PbPb data, while a strong system size dependence is observed for correlations of v2 and v4 harmonics. These new data provide important insights to the origin of collectivity observed in small collision systems.
Figures & Tables Summary Additional Figures References CMS Publications
Figures

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Figure 1:
The v2, v3 and v4 harmonics from long-range two-particle correlations for 0.3 <pT< 3 GeV/c as a function of Nofflinetexttrk in pp at s= 13 TeV, pPb at sNN= 8.16 TeV, and PbPb at sNN= 5.02 TeV. The lines show the vn results before subtraction of low-multiplicity correlations.

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Figure 2:
The SC for the second and third harmonic (red points) and the second and forth harmonic (blue points) as a function of Nofflinetexttrk in pp at s= 13 TeV, pPb at sNN= 5.02 and 8.16 TeV, and PbPb at sNN= 5.02 TeV.

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Figure 3:
The SC for the second and third harmonic (left) and the second and forth harmonic (right) normalized by <v22><v23> and <v22><v24> from dihardon correlations respectively. The pT range for considered tracks is 0.3 <pT< 3 GeV/c and the results are shown as a function of Nofflinetexttrk in pp at s= 13 TeV, pPb at sNN= 8.16 TeV, and PbPb at sNN= 5.02 TeV.
Tables

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Table 1:
Summary of systematic uncertainties for vn harmonics derived from two-particle correlations in pPb 8.16 TeV and PbPb 5.02 TeV.

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Table 2:
Summary of systematic uncertainties for SC in pPb 8.16 TeV and PbPb 5.02 TeV.
Summary
First measurement of azimuthal anisotropy Fourier harmonics and event-by-event correlations of different harmonics orders in pPb collisions at sNN= 8.16 TeV is presented with data collected by the CMS experiment at CERN. The v2-v4 Fourier harmonics are extracted from long-range two-particle correlations as a function of event multiplicity, and found to be similar to lower energy pPb sNN= 5.02 TeV data. The pPb data are compared to pp s= 13 TeV and PbPb sNN= 5.02 TeV systems. Using four-particle cumulant technique, correlations of different harmonic orders are obtained, where an anti-correlation is observed between v2 and v3 in pPb collisions, while v2 and v4 are positively correlated. This behavior is similar between pPb and PbPb systems. Normalized correlation coefficients of the 2nd and 3rd order are found to be quantitatively similar between pPb and PbPb systems. For the 2nd and 4th order, they are slightly higher in pPb than in PbPb. This result may point to a different contribution from the initial-state correlations or different transport properties like the shear viscosity to entropy ratio (η/s). The pp normalized symetric cumulant result shows a similar trend at high multiplicity compared to pPb and PbPb systems but the statistical uncertainties are too large to make a quantitative statement. The results presented in this paper provide further strong evidence of a similar origin of collectivity observed in small and large hadronic collision systems, and also impose novel constraints on the theoretical calculations.
Additional Figures

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Additional Figure 1:
Level-1 (L1) trigger efficiency as a function of Nofflinetrk for high-multiplicity event selection in pPb 8.16 TeV.

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Additional Figure 2:
High Level Trigger (HLT) efficiency as a function of Nofflinetrk for high-multiplicity event selection in pPb 8.16 TeV.

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Additional Figure 3:
L1+HLT efficiency as a function of Nofflinetrk for high-multiplicity event selection in pPb 8.16 TeV.

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Additional Figure 4:
2-D two-particle correlation function for 1 <ptrigT< 3 GeV/c, 1 <passocT< 3 GeV/c in 8.16 TeV pPb data with 330 <Nofflinetrk< 350 for charged particles.

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Additional Figure 5:
1-D two-particle correlation function for 1 <ptrigT< 3 GeV/c, 1 <passocT<3 GeV/c, average over |Δη|> 2, in 8.16 TeV pPb data with 330 <Nofflinetrk< 350 for charged particles. 2-particle Vn coefficients obtained from a Fourier fit of the distribution are also shown.

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Additional Figure 6:
SC(2,3) and SC(2,4) as a function of centrality from CMS (full) compared with ALICE data (open) with the same kinematic cuts.

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Additional Figure 7:
The SC for the second and third harmonic (left) and the second and forth harmonic (right) normalized by unsubtracted <v22>.<v23> and <v22>.<v24> from dihadron correlations respectively. The pT range for considered tracks is 0.3 <pT< 3 GeV/c and the results are shown as a function of Nofflinetrk in pp at s= 13 TeV, pPb at sNN= 8.16 TeV, and {\text {PbPb}} at sNN= 5.02 TeV.
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