Showing 25 of 3282 results
We report on a measurement of the differential cross sections of inclusive$K^{\pm}_{890}$production in$\sigma^-, pi^-$and ne
The production cross sections for K*+- per nucleus and per nucleon for the SIGMA- beam.
The production cross sections for K*+- per nucleus and per nucleon for the PI- beam.
The production cross sections for K*+- per nucleus and per nucleon for the NEUTRON- beam.
The differential cross sections for K*- production as a function of XL.
The differential cross sections for K*+ production as a function of XL.
Differential production cross sections for K*- as a function of PT**2.
Differential production cross sections for K*+ as a function of PT**2.
Differential cross sections for K*- AND K*+ production from a neutron beam as a function of PT**2.
The production of the Lambda and Sigma0 hyperons has been measured via the pp->pK+Lambda / Sigma0 reaction at the internal COSY-11 facility in the excess energy range between 14 and 60 MeV. The transition of the Lambda/Sigma0 cross section ratio from about 28 at Q<=13 MeV to the high energy level of about 2.5 is covered by the data showing a strong decrease of the ratio between 10 and 20 MeV excess energy. Effects from the final state interactions in the p-Sigma0 channel seem to be much smaller compared to the p-Lambda one. Estimates of the effective range parameters are given for the N-Lambda and the N-Sigma systems.
Cross section for LAMBDA production.. Statistical errors only.
Cross section for SIGMA0 production.. Statistical errors only.
Energy dependence of the LAMBDA/SIGMA0 ratio.
The angular distributions of the reactione+e−→μ+μ− ande+e+→τ+τ− have been measured between\(\sqrt s= 50\) and 60.8 GeV with the VENUS detector at TRISTAN. The average total cross section and the forward-backward charge asymmetry for μ-pair production are observed to be 28.3±1.4±0.8 pb and (−29.0−4.8+5.0±0.5)%, and those for τ-pair production are 27.6±1.7±1.0 pb and (−32.8−6.2+6.4±1.5)% at\(\langle \sqrt s \rangle \). These values are consistent with the predictions of the standard model of electroweak interactions.
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Results on the production cross sections ofW andZ bosons detected in the UA2 experiment are given based on a large sample ofW→eν andZ→e+e− decays. The measured cross sections are σWe = 660±15(stat)±37(syst)pb, σZe = 70.4±5.5(stat)±4.0(syst)pb and their ratioR=9.38−0.72+0.82(stat)±0.25(syst). In the framework of the Standard Model, the measured value ofR is used to determine the total width of theW, Γ(W)=2.30±0.19(stat)±0.06(syst) GeV.
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Inclusive and semi-inclusive cross sections and distributions of γ's and π0's inK+p interactions at 70 GeV/c are presented. The results are compared to other experiments and to the Lund model for low-pT hadron collisions.
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Axis error includes +- 0.0/0.0 contribution (?////).
The proton-to-pion ratios measured in the BRAHMS experiment for Au+Au and p+p collisions at $\sqrt{s_{NN}}$ = 62.4 and 200 GeV are presented as a function of transverse momentum and collision centrality at selected pseudorapidities in the range of 0 to 3.8. A strong pseudorapidity dependence of these ratios is observed. We also compare the magnitude and p_T-dependence of the p/pi ratios measured in Au+Au collisions at \rootsnn{200} and $\eta \approx 2.2$ with the same ratio measured at \rootsnn{62.4} and $\eta = 0$. The great similarity found between these ratios throughout the whole p_T range (up to 2.2 GeV/$c$) is consistent with particle ratios in A+A collisions being described with grand-canonical distributions characterized by the baryo-chemical potential \mibn. At the collision energy of 62.4 GeV, we have observed a unique point in pseudorapidity, $\eta = 3.2$, where the p/pi+ ratio is independent of the collision system size in a wide p_T-range of $0.3 \le p_{T} \le 1.8$ GeV/$c$.
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{p}\mathrm{p}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{p}\mathrm{p}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{p}\mathrm{p}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{p}\mathrm{p}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{p}\mathrm{p}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$
$\overline{\mathrm{p}}/\mathrm{\pi}^{-}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{-}$, $\overline{\mathrm{p}}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
$\overline{\mathrm{p}}/\mathrm{\pi}^{-}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{-}$, $\overline{\mathrm{p}}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
$\overline{\mathrm{p}}/\mathrm{\pi}^{-}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{-}$, $\overline{\mathrm{p}}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
$\overline{\mathrm{p}}/\mathrm{\pi}^{-}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{-}$, $\overline{\mathrm{p}}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
$\overline{\mathrm{p}}/\mathrm{\pi}^{-}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{-}$, $\overline{\mathrm{p}}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
$\overline{\mathrm{p}}/\mathrm{\pi}^{-}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{-}$, $\overline{\mathrm{p}}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
$\overline{\mathrm{p}}/\mathrm{\pi}^{-}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{-}$, $\overline{\mathrm{p}}$ in $\mathrm{p}\mathrm{p}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$
$\overline{\mathrm{p}}/\mathrm{\pi}^{-}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{-}$, $\overline{\mathrm{p}}$ in $\mathrm{p}\mathrm{p}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$
$\overline{\mathrm{p}}/\mathrm{\pi}^{-}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{-}$, $\overline{\mathrm{p}}$ in $\mathrm{p}\mathrm{p}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$
$\overline{\mathrm{p}}/\mathrm{\pi}^{-}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{-}$, $\overline{\mathrm{p}}$ in $\mathrm{p}\mathrm{p}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$
$\overline{\mathrm{p}}/\mathrm{\pi}^{-}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{-}$, $\overline{\mathrm{p}}$ in $\mathrm{p}\mathrm{p}$ at $\sqrt{s}=200\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=62.4\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{p}\mathrm{p}$ at $\sqrt{s}=62.4\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=62.4\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=62.4\,\mathrm{Ge\!V}$
$\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{+}$, $\mathrm{p}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=62.4\,\mathrm{Ge\!V}$
$\overline{\mathrm{p}}/\mathrm{\pi}^{-}$, $\mathrm{p}/\mathrm{\pi}^{+}$ versus $p_{\mathrm{T}}$ for $\mathrm{\pi}^{-}$, $\mathrm{\pi}^{+}$, $\mathrm{p}$, $\overline{\mathrm{p}}$ in $\mathrm{Au}-\mathrm{Au}$ at $\sqrt{s_{\mathrm{NN}}}=200\,\mathrm{Ge\!V}$
Using data collected with the CLEO II detector at the Cornell Electron Storage Ring, we determine the ratio R(chrg) for the mean charged multiplicity observed in Upsilon(1S)->gggamma events, to the mean charged multiplicity observed in e+e- -> qqbar gamma events. We find R(chrg)=1.04+/-0.02+/-0.05 for jet-jet masses less than 7 GeV.
No description provided.
Single particles and jets in deeply inelastic scattering at low x are measured with the H1 detector in the region away from the current jet and towards the proton remnant, known as the forward region. Hadronic final state measurements in this region are expected to be particularly sensitive to QCD evolution effects. Jet cross-sections are presented as a function of Bjorken-x for forward jets produced with a polar angle to the proton direction, theta, in the range 7 < theta < 20 degrees. Azimuthal correlations are studied between the forward jet and the scattered lepton. Charged and neutral single particle production in the forward region are measured as a function of Bjorken-x, in the range 5 < theta < 25 degrees, for particle transverse momenta larger than 1 GeV. QCD based Monte Carlo predictions and analytical calculations based on BFKL, CCFM and DGLAP evolution are compared to the data. Predictions based on the DGLAP approach fail to describe the data, except for those which allow for a resolved photon contribution.
Forward Jet cross section. Axis error includes +- 7/7 contribution (Dependence of the model used to correct the data).
Forward Di-jet cross section. Axis error includes +- 7/7 contribution (Dependence of the model used to correct the data).
Data from Figure 3a on charged particle production
Data from Figure 3b on charged pion production. Data correspond to charged particle production, corrected to the contribution from (PI+ + PI-)/2.
Data from Figure 3b on charged pion production. Data correspond to charged particle production, corrected to the contribution from (PI+ + PI-)/2.
Data from Figure 3c on charged pion production. Data correspond to charged particle production, corrected to the contribution from (PI+ + PI-)/2.
Data from Figure 3d on charged pion production. Data correspond to charged particle production, corrected to the contribution from (PI+ + PI-)/2.
Data from Figure 4a on forward jet production differential in x, low PT
Data from Figure 4a on forward jet production differential in x, high PT
Data from Figure 5a on forward jet production differential in delta(phi), low x
Data from Figure 5b on forward jet production differential in delta(phi), high x
The cross section of W-boson pair-production is measured with the L3 detector at LEP. In a data sample corresponding to a total luminosity of 629.4/pb, collected at centre-of-mass energies ranging from 189 to 209 GeV, 9834 four-fermion events with W bosons decaying into hadrons or leptons are selected. The total cross section is measured with a precision of 1.4 % and agrees with the Standard Model expectation. Assuming charged-lepton universality, the branching fraction for hadronic W-boson decays is measured to be: Br(W-->hadrons) = 67.50 +- 0.42 (stat.) +- 0.30(syst.) %, in agreement with the Standard Model. Differential cross sections as a function of the W- production angle are also measured for the semi-leptonic channels qqev and qqmv.
Measured cross section for the process E+ E- --> LEPTON NU LEPTON NU.
Measured cross section for the process E+ E- --> QUARK QUARKBAR ELECTRON NEUTRINO.
Measured cross section for the process E+ E- --> QUARK QUARKBAR MUON NEUTRINO.
Measured cross section for the process E+ E- --> QUARK QUARKBAR TAU NEUTRINO.
Measured cross section for the process E+ E- --> QUARK QUARKBAR QUARK QUARKBAR.
Measured value of the QUARK QUARKBAR cross section.
Measured values of the cross section for W+ W- production into the fully leptonic decay mode summed over all lepton modes and assuming charged lepton universality.
Measured values of the cross section for W+ W- production into semi leptonic decay mode summed over all lepton flavours and assuming charged lepton universality.
Measured values of the cross section for W+ W- production in the fully hadronic decay mode.
The measured values of the E+ E- --> W+ W- cross section summed over all decay modes.
Angular distributions of the W+ W- cross sections resulting from the sum of the (QUARK QUARKBAR ELECTRON NEUTRINO) and the (QUARK QUARKBAR MUON NEUTRINO) cross sections.
A search for single top quark production is performed in e^\pm p collisions at HERA. The search exploits data corresponding to an integrated luminosity of 118.3 pb^-1. A model for the anomalous production of top quarks in a flavour changing neutral current process involving a t-u-gamma coupling is investigated. Decays of top quarks into a b quark and a W boson are considered in the leptonic and the hadronic decay channels of the W. Both a cut-based analysis and a multivariate likelihood analysis are performed to discriminate anomalous top quark production from Standard Model background processes. In the leptonic channel, 5 events are found while 1.31 \pm 0.22 events are expected from the Standard Model background. In the hadronic channel, no excess above the expectation for Standard Model processes is found. These observations lead to a cross section \sigma (ep -> e t X) = 0.29 +0.15 -0.14 pb at \sqrt{s} = 319 GeV. Alternatively, assuming that the observed events are due to a statistical fluctuation, upper limits of 0.55 pb on the anomalous top production cross section and of 0.27 on the t-u-gamma coupling \kappa_{t-u-gamma} are established at the 95% confidence level.
Cross section from a combination of electron, muon and hadron channels.
Exclusive rho rho production in two-photon collisions involving a single highly virtual photon is studied with data collected at LEP at centre-of-mass energies 89GeV < \sqrt{s} < 209GeV with a total integrated luminosity of 854.7pb^-1 The cross section of the process gamma gamma^* -> rho rho is determined as a function of the photon virtuality, Q^2 and the two-photon centre-of-mass energy, Wgg, in the kinematic region: 1.2GeV^2 < Q^2 < 30GeV^2 and 1.1GeV < Wgg < 3GeV.
Production cross sections as a function of Q**2. The differential cross sections are corrected to the centre of each bin.
Production cross section for the two photon data as a function of Q**2.
Differential cross section for non-resonance and RHO0 RHO0 data corrected to the centre of each bin.
Cross sections as a function of W for the lower Q**2, Z pole, data.
Cross sections as a function of W for the high Q**2 data.
Cross sections for the two photon RHO0 RHO0 and non-resonance data for the lower Q**2, Z pole, data.
Cross sections for the two photon RHO0 RHO0 and non-resonance data for the higher Q**2 data.
Dihadron azimuthal correlations containing a high transverse momentum ($p_T$) trigger particle are sensitive to the properties of the nuclear medium created at RHIC through the strong interactions occurring between the traversing parton and the medium, i.e. jet-quenching. Previous measurements revealed a strong modification to dihadron azimuthal correlations in Au+Au collisions with respect to p+p and d+Au collisions. The modification increases with the collision centrality, suggesting a path-length or energy density dependence to the jet-quenching effect. This paper reports STAR measurements of dihadron azimuthal correlations in mid-central (20-60%) Au+Au collisions at $\sqrt{s_{_{\rm NN}}}=200$ GeV as a function of the trigger particle's azimuthal angle relative to the event plane, $\phi_s=|\phi_t-\psi_{\rm EP}|$. The azimuthal correlation is studied as a function of both the trigger and associated particle $p_T$. The subtractions of the combinatorial background and anisotropic flow, assuming Zero Yield At Minimum (ZYAM), are described. The correlation results are first discussed with subtraction of the even harmonic (elliptic and quadrangular) flow backgrounds. The away-side correlation is strongly modified, and the modification varies with $\phi_s$, with a double-peak structure for out-of-plane trigger particles. The near-side ridge (long range pseudo-rapidity $\Delta\eta$ correlation) appears to drop with increasing $\phi_s$ while the jet-like component remains approximately constant. The correlation functions are further studied with subtraction of odd harmonic triangular flow background arising from fluctuations. It is found that the triangular flow, while responsible for the majority of the amplitudes, is not sufficient to explain the $\phi_s$-dependence of the ridge or the away-side double-peak structure. ...
red data points
black histogram
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
dN/deta phis=045 deg, pt=0.151 GeV/c
dN/deta phis=045 deg, pt=0.153 GeV/c
dN/deta phis=090 deg, pt=0.51 GeV/c
dN/deta phis=090 deg, pt=12 GeV/c
dN/deta phis=4590 deg, pt=0.151 GeV/c
sigma vs phis pt=0.151 GeV/c
sigma vs phis pt=0.153 GeV/c
sigma vs phis pt=0.51 GeV/c
sigma vs phis pt=12 GeV/c
sigma vs pt phis=045 deg
sigma vs pt phis=090 deg
sigma vs pt phis=4590 deg
background uncertainty caps in the figure
flow uncertainty curves in the figure
leadage uncertainty arrows in the figure
total uncertainty boxes in the figure
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
0^{o} < phi_{s} < 45^{o}
45^{o} < phi_{s} < 90^{o}
Previous in-plane result published in 2004
Previous out-of-plane result published in 2004
3<p_{\text{T}}^{(t)}<4, 1<p_{\text{T}}^{(a)}<2 GeV/c, 0^{o} < phi_{s} < 45^{o}
3<p_{\text{T}}^{(t)}<4, 1<p_{\text{T}}^{(a)}<2 GeV/c, 45^{o} < phi_{s} < 90^{o}
3<p_{\text{T}}^{(t)}<4, 2<p_{\text{T}}^{(a)}<3 GeV/c, 0^{o} < phi_{s} < 45^{o}
3<p_{\text{T}}^{(t)}<4, 2<p_{\text{T}}^{(a)}<3 GeV/c, 45^{o} < phi_{s} < 90^{o}
4<p_{\text{T}}^{(t)}<6, 1<p_{\text{T}}^{(a)}<2 GeV/c, 0^{o} < phi_{s} < 45^{o}
4<p_{\text{T}}^{(t)}<6, 1<p_{\text{T}}^{(a)}<2 GeV/c, 45^{o} < phi_{s} < 90^{o}
4<p_{\text{T}}^{(t)}<6, 2<p_{\text{T}}^{(a)}<3 GeV/c, 0^{o} < phi_{s} < 45^{o}
4<p_{\text{T}}^{(t)}<6, 2<p_{\text{T}}^{(a)}<3 GeV/c, 45^{o} < phi_{s} < 90^{o}
3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
3<p_{\text{T}}^{(t)}<4 GeV/c
3<p_{\text{T}}^{(t)}<4 GeV/c, 0^{o}15^{o}
3<p_{\text{T}}^{(t)}<4 GeV/c, 75^{o}90^{o}
Cone region, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
one region, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
one region, 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
one region, 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
i region, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
Pi region, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
i region, 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
i region, 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
d+Au, 3<p_{\text{T}}^{(t)}<4 GeV/c
20-60%, 3<p_{T}^{(t)}<4 GeV/c, (a) 0^{o}<#phi_{s}<15^{o}
20-60%, 3<p_{T}^{(t)}<4 GeV/c, (b) 75^{o}<#phi_{s}<90^{o}
20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, (a) 0^{o}<phi_{s}<15^{o}
20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, (b) 75^{o}<phi_{s}<90^{o}
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 0, jet
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 1, jet
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 2, jet
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 3, jet
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 4, jet
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 5, jet
1<p_{\text{T}}^{(a)}<2 GeV/c, jet
0-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/, slice 0, ridge
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 1, ridge
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 2, ridge
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 3, ridge
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 4, ridge
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 5, ridge
1<p_{\text{T}}^{(a)}<2 GeV/c, ridge
jet (Deltaphi|<1.0, |Deltaeta|<0.7) 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
jet (Deltaphi|<1.0, |Deltaeta|<0.7) 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
ridge (Deltaphi|<1.0, |Deltaeta|>0.7) 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
ridge (Deltaphi|<1.0, |Deltaeta|>0.7) 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
ridge (Deltaphi|<1.0, |Deltaeta|>0.7) 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
ridge (Deltaphi|<1.0, |Deltaeta|>0.7) 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
3<p_{\text{T}}^{(t)}<4 GeV/c Ridge (75^{o}<|phi_{s}|<90^{o}) / Ridge (0^{o}<|phi_{s}|<15^{o})
4<p_{\text{T}}^{(t)}<6 GeV/c Ridge (75^{o}<|phi_{s}|<90^{o}) / Ridge (0^{o}<|phi_{s}|<15^{o})
3<p_{\text{T}}^{(t)}<4 GeV/c Ridge (30^{o}<|phi_{s}|<45^{o}) / Ridge (0^{o}<|phi_{s}|<15^{o})
4<p_{\text{T}}^{(t)}<6 GeV/c Ridge (30^{o}<|phi_{s}|<45^{o}) / Ridge (0^{o}<|phi_{s}|<15^{o})
3<p_{\text{T}}^{(t)}<4 GeV/c Ridge (0^{o}<|phi_{s}|<15^{o}) / Jet (0^{o}<|phi_{s}|<15^{o})
4<p_{\text{T}}^{(t)}<6 GeV/c Ridge (0^{o}<|phi_{s}|<15^{o}) / Jet (0^{o}<|phi_{s}|<15^{o})
3<p_{\text{T}}^{(t)}<4 GeV/c, cone region
4<p_{\text{T}}^{(t)}<6 GeV/c, cone region
3<p_{\text{T}}^{(t)}<4 GeV/c, jetlike
4<p_{\text{T}}^{(t)}<6 GeV/c, jetlike
3<p_{\text{T}}^{(t)}<4 GeV/c, pi region
4<p_{\text{T}}^{(t)}<6 GeV/c, pi region
3<p_{\text{T}}^{(t)}<4 GeV/c, ridge
4<p_{\text{T}}^{(t)}<6 GeV/c, ridge
fig17_ampl_pt_inclusive
3<p_{\text{T}}^{(t)}<4 GeV/c, 0^{o}<phi_{s}<45^{o}, cone region
3<p_{\text{T}}^{(t)}<4 GeV/c, 0^{o}<phi_{s}<45^{o}, jetlike
3<p_{\text{T}}^{(t)}<4 GeV/c, 0^{o}<phi_{s}<45^{o}, pi region
3<p_{\text{T}}^{(t)}<4 GeV/c, 0^{o}<phi_{s}<45^{o}, pi region ridge
3<p_{\text{T}}^{(t)}<4 GeV/c, 0^{o}<phi_{s}<45^{o}, ridge
3<p_{\text{T}}^{(t)}<4 GeV/c, 45^{o}<phi_{s}<90^{o}, cone region
3<p_{\text{T}}^{(t)}<4 GeV/c, 45^{o}<phi_{s}<90^{o}, jetlike
3<p_{\text{T}}^{(t)}<4 GeV/c, 45^{o}<phi_{s}<90^{o}, pi region
3<p_{\text{T}}^{(t)}<4 GeV/c, 45^{o}<phi_{s}<90^{o}, pi region ridge
3<p_{\text{T}}^{(t)}<4 GeV/c, 45^{o}<phi_{s}<90^{o}, ridge
4<p_{\text{T}}^{(t)}<6 GeV/c, 0^{o}<phi_{s}<45^{o}, cone region
4<p_{\text{T}}^{(t)}<6 GeV/c, 0^{o}<phi_{s}<45^{o}, jetlike
4<p_{\text{T}}^{(t)}<6 GeV/c, 0^{o}<phi_{s}<45^{o}, pi region
4<p_{\text{T}}^{(t)}<6 GeV/c, 0^{o}<phi_{s}<45^{o}, pi region ridge
4<p_{\text{T}}^{(t)}<6 GeV/c, 0^{o}<phi_{s}<45^{o}, ridge
4<p_{\text{T}}^{(t)}<6 GeV/c, 45^{o}<phi_{s}<90^{o}, cone region
4<p_{\text{T}}^{(t)}<6 GeV/c, 45^{o}<phi_{s}<90^{o}, jetlike
4<p_{\text{T}}^{(t)}<6 GeV/c, 45^{o}<phi_{s}<90^{o}, pi region
4<p_{\text{T}}^{(t)}<6 GeV/c, 45^{o}<phi_{s}<90^{o}, pi region ridge
4<p_{\text{T}}^{(t)}<6 GeV/c, 45^{o}<phi_{s}<90^{o}, ridge
jetlike eta sigma
cone peak phi sigma
jetlike phi sigma
ridge phi sigma
jetlike eta sigma
cone peak phi sigma
jetlike phi sigma
ridge phi sigma
dAu jetlike eta sigma
dAu jetlike phi sigma
cone peak centroid
cone peak centroid
cone peak centroid
cone peak centroid
cone peak centroid
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
v_{2} /3
v_{3}
v_{4}
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
background subtracted correlation with upper flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 0
background subtracted correlation with upper flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 1
background subtracted correlation with upper flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 2
background subtracted correlation with upper flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 3
background subtracted correlation with upper flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 4
background subtracted correlation with upper flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 5
background subtracted correlation with upper flow systematic uncertainty Difference of the above results default results in Fig.21, slice 0
background subtracted correlation with upper flow systematic uncertainty Difference of the above results default results in Fig.21, slice 1
background subtracted correlation with upper flow systematic uncertainty Difference of the above results default results in Fig.21, slice 2
background subtracted correlation with upper flow systematic uncertainty Difference of the above results default results in Fig.21, slice 3
background subtracted correlation with upper flow systematic uncertainty Difference of the above results default results in Fig.21, slice 4
background subtracted correlation with upper flow systematic uncertainty Difference of the above results default results in Fig.21, slice 5
background subtracted correlation with lower flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 0
background subtracted correlation with lower flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 1
background subtracted correlation with lower flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 2
background subtracted correlation with lower flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 3
background subtracted correlation with lower flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 4
background subtracted correlation with lower flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 5
background subtracted correlation with lower flow systematic uncertainty Difference of the above results default results in Fig.21, slice 0
background subtracted correlation with lower flow systematic uncertainty Difference of the above results default results in Fig.21, slice 1
background subtracted correlation with lower flow systematic uncertainty Difference of the above results default results in Fig.21, slice 2
background subtracted correlation with lower flow systematic uncertainty Difference of the above results default results in Fig.21, slice 3
background subtracted correlation with lower flow systematic uncertainty Difference of the above results default results in Fig.21, slice 4
background subtracted correlation with lower flow systematic uncertainty Difference of the above results default results in Fig.21, slice 5
background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles, slice 0
background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles, slice 1
background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles, slice 2
background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles, slice 3
background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles, slice 4
background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles, slice 5
background subtracted correlation Difference of the above results default results in Fig.21, slice 0
background subtracted correlation Difference of the above results default results in Fig.21, slice 1
background subtracted correlation Difference of the above results default results in Fig.21, slice 2
background subtracted correlation Difference of the above results default results in Fig.21, slice 3
background subtracted correlation Difference of the above results default results in Fig.21, slice 4
background subtracted correlation Difference of the above results default results in Fig.21, slice 5
d+Au background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles
difference from default results, slice 0
difference from default results, slice 1
difference from default results, slice 2
difference from default results, slice 3
difference from default results, slice 4
difference from default results, slice 5
raw signal
bkgd <v2t*v2>
bkgd <v2t>*<v2> (previous inclusive analysis)
bkgd <v2t*v2> subtracted
bkgd <v2t>*<v2> subtracted (previous inclusive analysis)
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
d+Au raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
d+Au raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
d+Au raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
d+Au raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
d+Au raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |#Delta#eta|>0.7, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
d+Au jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
d+Au jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
d+Au jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
d+Au jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
jet correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
d+Au jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c
d+Au jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c
d+Au jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c
d+Au jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c
d+Au jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c
d+Au jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
jet correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
Results are presented for six nuclei from Be to Pb on the structure function ratios F 2 A / F 2 C ( x ) and their A dependence in deep inelastic muon scattering at 200 GeV incident muon energy. The data cover the kinematic range 0.01 < x < 0.8 with Q 2 ranging from 2 to 70 GeV 2 . The A dependence of nuclear structure function ratios is parametrised and compared to various models.
Additional normalisation error of 0.002 in the ratio.
Additional normalisation error of 0.002 in the ratio.
Additional normalisation error of 0.003 in the ratio.
Additional normalisation error of 0.002 in the ratio.
Additional normalisation error of 0.002 in the ratio.
Additional normalisation error of 0.002 in the ratio.
Transverse particle momenta have been measured ine+e− annihilation into hadrons at c.m. energies between 9.4 and 31.6 GeV. The data are fully corrected for detector effects and radiation in the initial state. A comparison is made with recent QCD calculations.
MEASUREMENTS MADE WITH RESPECT TO THE SPHERICITY AXIS.
MEASUREMENTS MADE WITH RESPECT TO THE THRUST AXIS.
MEASUREMENTS MADE WITH RESPECT TO THE MOST ENERGETIC PARTON AXIS.
The first search for narrow resonances decaying to three well-separated hadronic jets is presented. The search uses proton-proton collision data corresponding to an integrated luminosity of 138 fb$^{-1}$ at $\sqrt{s}$ = 13 TeV, collected at the CERN LHC. No significant deviations from the background predictions are observed between 1.75-9.00 TeV. The results provide the first mass limits on a right-handed boson Z$_{\mathrm{R}}$ decaying to three gluons, an excited quark decaying via a vector boson to three quarks, as well as updated limits on a Kaluza-Klein gluon decaying via a radion to three gluons.
Observed and expected (background-only fitted) invariant mass spectra of trijet events. Data spectra from three years are fitted separately and the sum is shown in the figure. The fitting function used is ${ d N}/{ d m} = p_{0}(1-x)^{p_{1}}/x^{\sum_{i=2}^{3} p_{i}\log^{i-2}(x)}$. The fitted parameters are $p_{1} = 7.350, p_{2} = 6.926, p_{3} = 0.388$ for 2016, $p_{1} = 8.308, p_{2} = 5.931, p_{3} = 0.167$ for 2017 and $p_{1} = 8.770, p_{2} = 5.617, p_{3} = 0.106$ for 2018. $p_{0}$ is the normalization parameter and its exact value is irrelevant.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to ggg) \mathcal{A}$ for a 3-body decay trijet resonance with $\Gamma_{X}\sim 3\% m_{X}$. The acceptance $\mathcal{A}$ is defined as $\mathcal{A} = N$(events with $m_{X}^{GEN} > 85\% m_{X}^{input}$) / $N$(events generated in the full phase space defined by the CMS default generator settings). Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions assuming SM-like couplings are depicted with the red curve.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to ggg) \mathcal{A}$ for a 3-body decay trijet resonance with $\Gamma_{X}\sim 0.01\% m_{X}$. The acceptance $\mathcal{A}$ is defined as $\mathcal{A} = N$(events with $m_{X}^{GEN} > 85\% m_{X}^{input}$) / $N$(events generated in the full phase space defined by the CMS default generator settings). Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions are depicted with the red curve.
Observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(gg)g) \mathcal{A}$ for a cascade decay trijet resonance. The acceptance $\mathcal{A}$ is defined as $\mathcal{A} = N$(events with $m_{X}^{GEN} > 85\% m_{X}^{input}$) / $N$(events generated in the full phase space defined by the CMS default generator settings). Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Mass exclusion ranges of the benchmark signal scenarios are depicted with hatched areas inside the black contours.
Observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(qq)q) \mathcal{A}$ for a cascade decay trijet resonance. The acceptance $\mathcal{A}$ is defined as $\mathcal{A} = N$(events with $m_{X}^{GEN} > 85\% m_{X}^{input}$) / $N$(events generated in the full phase space defined by the CMS default generator settings). Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Mass exclusion ranges of the benchmark signal scenarios are depicted with hatched areas inside the black contours.
Efficiencies of the selection requirements on the benchmark signal processes: $Z_{R} \to ggg$ with nominal width ($\Gamma_{X}/m_{X}\sim 3\%$). A value of -1 means that the corresponding efficiency is not calculated for this year.
Efficiencies of the selection requirements on the benchmark signal processes: $Z_{R} \to ggg$ with narrow width ($\Gamma_{X}/m_{X}\sim 0.01\%$). A value of -1 means that the corresponding efficiency is not calculated for this year.
Efficiencies of the selection requirements on the benchmark signal processes: $G_{KK} \to {\varphi}(gg)g$, where $\varphi$ is the radion. A value of -1 means that the corresponding efficiency is not calculated for this year.
Efficiencies of the selection requirements on the benchmark signal processes: $q^{*} \to V(qq)q$, where $V$ is a beyond-the-SM vector boson. A value of -1 means that the corresponding efficiency is not calculated for this year.
Acceptance of the signal selection requirement $m_{X}^{\text{GEN}}/m_{X}^{\text{input}} > 85\%$ on the benchmark signal process $Z_{R} \to ggg$. The acceptance is defined as $\mathcal{A} = N$(events with $m_{X}^{\text{GEN}}/m_{X}^{\text{input}} > 85\%$)/$N$(events generated in the full phase space defined by the CMS default generator settings).
Acceptance of the signal selection requirement $m_{X}^{\text{GEN}}/m_{X}^{\text{input}} > 85\%$ on the benchmark signal process $G_{KK} \to {\varphi}(gg)g$.
Acceptance of the signal selection requirement $m_{X}^{\text{GEN}}/m_{X}^{\text{input}} > 85\%$ on the benchmark signal process $q^{*} \to V(qq)q$.
Observed local significance for a 3-body decay $ggg$ resonance, shown for resonances with nominal width (blue solid line) and narrow width (red dashed line).
Observed local significance for a cascade decay $ggg$ resonance.
Observed local significance for a cascade decay $qqq$ resonance.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(gg)g) \mathcal{A}$ for a cascade decay trijet resonance with $m_{Y} / m_{X} = 0.2$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(gg)g) \mathcal{A}$ for a cascade decay trijet resonance with $m_{Y} / m_{X} = 0.3$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(gg)g) \mathcal{A}$ for a cascade decay trijet resonance with $m_{Y} / m_{X} = 0.4$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(gg)g) \mathcal{A}$ for a cascade decay trijet resonance with $m_{Y} / m_{X} = 0.5$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(gg)g) \mathcal{A}$ for a cascade decay trijet resonance with $m_{Y} / m_{X} = 0.6$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(gg)g) \mathcal{A}$ for a cascade decay trijet resonance with $m_{Y} / m_{X} = 0.7$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(gg)g) \mathcal{A}$ for a cascade decay trijet resonance with $m_{Y} / m_{X} = 0.8$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(qq)q) \mathcal{A}$ for a cascade decay trijet resonance $m_{Y} / m_{X} = 0.2$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(qq)q) \mathcal{A}$ for a cascade decay trijet resonance with $m_{Y} / m_{X} = 0.3$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(qq)q) \mathcal{A}$ for a cascade decay trijet resonance with $m_{Y} / m_{X} = 0.4$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(qq)q) \mathcal{A}$ for a cascade decay trijet resonance with $m_{Y} / m_{X} = 0.5$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(qq)q) \mathcal{A}$ for a cascade decay trijet resonance with $m_{Y} / m_{X} = 0.6$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(qq)q) \mathcal{A}$ for a cascade decay trijet resonance with $m_{Y} / m_{X} = 0.7$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal.
Expected and observed limits at 95% CL on $\sigma \mathcal{B} (X \to Y(qq)q) \mathcal{A}$ for a cascade decay trijet resonance with $m_{Y} / m_{X} = 0.8$. Only 2016 data are used to derive limits below 2.0 TeV because of higher trigger thresholds in 2017 and 2018. Theoretical predictions of the benchmark are depicted with the red curve. A value of -1 in the table means that the corresponding theoretical prediction is not calculated for this signal
Cut flow table of the selection requirments for the $Z_{R}$ model scenarios. Values shown are absolute efficiencies, e.g., values shown in the column of 'Efficiency ($\Delta_{R}^{max} < 3.0$)' represent the cumulative efficiencies achieved through all selection requirements applied up to and including the current selection criterion.
Cut flow table of the selection requirments for the $G_{KK}$ model scenarios. Values shown are absolute efficiencies, e.g., values shown in the column of 'Efficiency ($\Delta_{R}^{max} < 3.0$)' represent the cumulative efficiencies achieved through all selection requirements applied up to and including the current selection criterion.
Cut flow table of the selection requirments for the $q^{*}$ model scenarios. Values shown are absolute efficiencies, e.g., values shown in the column of 'Efficiency ($\Delta_{R}^{max} < 3.0$)' represent the cumulative efficiencies achieved through all selection requirements applied up to and including the current selection criterion.
Predicted production cross section of the benchmark signal process $pp \to Z_{R} \to ggg$.
Predicted production cross section of the benchmark signal process $pp \to G_{KK} \to \varphi(gg)g$.
Predicted production cross section of the benchmark signal process $pp \to q^{*} \to V(qq)q$.
A test of lepton flavor universality in B$^{\pm}$$\to$ K$^{\pm}\mu^+\mu^-$ and B$^{\pm}$$\to$ K$^{\pm}$e$^+$e$^-$ decays, as well as a measurement of differential and integrated branching fractions of a nonresonant B$^{\pm}$$\to$ K$^{\pm}\mu^+\mu^-$ decay are presented. The analysis is made possible by a dedicated data set of proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded in 2018, by the CMS experiment at the LHC, using a special high-rate data stream designed for collecting about 10 billion unbiased b hadron decays. The ratio of the branching fractions $\mathcal{B}$(B$^{\pm}$$\to$ K$^{\pm}\mu^+\mu^-$) to $\mathcal{B}$(B$^{\pm}$$\to$ K$^{\pm}$e$^+$e$^-$) is determined from the measured double ratio $R$(K) of these decays to the respective branching fractions of the B$^\pm$$\to$ J/$\psi$K$^\pm$ with J/$\psi$$\to$$\mu^+\mu^-$ and e$^+$e$^-$ decays, which allow for significant cancellation of systematic uncertainties. The ratio $R$(K) is measured in the range 1.1 $\lt q^2 \lt$ 6.0 GeV$^2$, where $q$ is the invariant mass of the lepton pair, and is found to be $R$(K) = 0.78$^{+0.47}_{-0.23}$, in agreement with the standard model expectation $R$(K) $\approx$ 1. This measurement is limited by the statistical precision of the electron channel. The integrated branching fraction in the same $q^2$ range, $\mathcal{B}$(B$^{\pm}$$\to$ K$^{\pm}\mu^+\mu^-$) = (12.42 $\pm$ 0.68) $\times$ 10$^{-8}$, is consistent with the present world-average value and has a comparable precision.
The differential $\text{B}^+ \to \text{K}^+\mu^+\mu^-$ branching fraction measured in the individual $q^2$ bins. The uncertainties in the yields are statistical uncertainties from the fit, while the branching fraction uncertainties include both the statistical and systematic components.
Differential branching fraction $d\mathcal{B}/dq^2$, with theoretical predictions obtained with the HEPFiT, SuperIso, Flavio, and EOS packages. The HEPFiT predictions are available only for $q^2 < 8\ \mathrm{GeV}^2$.
Relative uncertainties in the differential branching fraction measurement of $\mathrm{B}^+\to\mathrm{K}^+\mu^+\mu^-$ per $q^2$ bin.
Correlation matrix for the differential branching fraction extraction between different $q^2$ bins in the simultaneous fit.
The product of acceptance and efficiency ($A\epsilon$) of the $\mathcal{B}(\mathrm{B}^+\to\mathrm{K}^+\mu^+\mu^-)$ channel, as a function of the muon pair $q^2$, as measured in simulated signal events, after all the corrections applied. In the figure, regions corresponding to resonances are displayed with red markers.
Same as Table 5, but for the bins containing the J$\psi$ and $\psi$(2S) resonances.
Integrated branching fraction $\mathcal{B}(\mathrm{B}^\pm \to \mathrm{K}^\pm\mu^+\mu^-)$ in the low-$q^2$ region.
Ratio of branching fractions $\mathcal{B}(\text{B}^\pm \to \text{K}^\pm\mu^+\mu^-)$ to $\mathcal{B}(\text{B}^\pm \to \text{K}^\pm\text{e}^+\text{e}^-)$, determined from the measured double ratio $R$(K) of these decays to the respective branching fractions of the decay chains $\text{B}^\pm\to\text{J/}\psi\text{K}^\pm$ with $\text{J/}\psi\to\mu^+\mu^-$ and $\text{e}^+\text{e}^-$.
Negative log likelihood function from the fit profiled as a function of the inverse ratio $R(\mathrm{K})^{-1}$.
Using proton-proton collision data corresponding to an integrated luminosity of 140 fb$^{-1}$ collected by the CMS experiment at $\sqrt{s}$ = 13 TeV, the $\Lambda_\text{b}^0$$\to$ J/$\psi\Xi^-$K$^+$ decay is observed for the first time, with a statistical significance exceeding 5 standard deviations. The relative branching fraction, with respect to the $\Lambda_\text{b}^0$$\to$$\psi$(2S)$\Lambda$ decay, is measured to be $\mathcal{B}$($\Lambda_\text{b}^0$$\to$ J/$\psi\Xi^-$K$^+$)/$\mathcal{B}$( $\Lambda_\text{b}^0$$\to$$\psi$(2S)$\Lambda$) = [3.38 $\pm$ 1.02 $\pm$ 0.61 $\pm$ 0.03]%, where the first uncertainty is statistical, the second is systematic, and the third is related to the uncertainties in $\mathcal{B}$($\psi$(2S) $\to$ J/$\psi\pi^+\pi^-$) and $\mathcal{B}$($\Xi^-$ $\to$ $\Lambda\pi^-$).
The measured branching fraction ratio
Measurements of inclusive and normalized differential cross sections of the associated production of top quark-antiquark and bottom quark-antiquark pairs, ttbb, are presented. The results are based on data from proton-proton collisions collected by the CMS detector at a centre-of-mass energy of 13 TeV, corresponding to an integrated luminosity of 138 fb$^{-1}$. The cross sections are measured in the lepton+jets decay channel of the top quark pair, using events containing exactly one isolated electron or muon and at least five jets. Measurements are made in four fiducial phase space regions, targeting different aspects of the ttbb process. Distributions are unfolded to the particle level through maximum likelihood fits, and compared with predictions from several event generators. The inclusive cross section measurements of this process in the fiducial phase space regions are the most precise to date. In most cases, the measured inclusive cross sections exceed the predictions with the chosen generator settings. The only exception is when using a particular choice of dynamic renormalization scale, $\mu_\mathrm{R}=\frac{1}{2} \prod_{i=\mathrm{t, \bar{t}, b, \bar{b}}} m_{\mathrm{T},i}^{1/4}$, where $m_{\mathrm{T},i}^2=m_i^2+p^2_{\mathrm{T},i}$ are the transverse masses of top and bottom quarks. The differential cross sections show varying degrees of compatibility with the theoretical predictions, and none of the tested generators with the chosen settings simultaneously describe all the measured distributions.
Fiducial cross sections from the measurements of all observables, compared to predictions from different ttbb simulation approaches. For each of the normalized differential measurements the fiducial cross section in the respective phase space is also determined. In the paper only one representative observable is quoted for each fiducial phase space, while here the measured cross section with the uncertainties from the fit to the respective observable is summarized.
Compatibility of normalized differential cross section measurements with modeling predictions. The compatibility is quantified with z scores for each of the theoretical predictions, given the unfolded normalized differential cross sections and their covariances. A lower value indicates a better agreement between prediction and measurement. A value of z = 2 indicates a p-value of 5%. In the calculation of the z score only the measurement uncertainties and the statistical uncertainties of the modeling predictions are taken into account
Normalized differential cross section of $|\eta(\mathrm{b}^{\mathrm{add.}}_{1})|$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $p_{\mathrm{T}}(\mathrm{b}^{\mathrm{add.}}_{1})$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $|\eta(\mathrm{b}^{\mathrm{add.}}_{2})|$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $p_{\mathrm{T}}(\mathrm{b}^{\mathrm{add.}}_{2})$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $|\eta(\mathrm{b}\mathrm{b}^{\mathrm{add.}})|$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $\Delta\mathrm{R}(\mathrm{b}\mathrm{b}^{\mathrm{add.}})$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $\mathrm{m}(\mathrm{b}\mathrm{b}^{\mathrm{add.}})$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $p_{\mathrm{T}}(\mathrm{b}\mathrm{b}^{\mathrm{add.}})$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $\Delta\mathrm{R}_{\mathrm{b}\mathrm{b}}^{\mathrm{avg}}$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $|\eta(\mathrm{b}_{3})|$ in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space.
Normalized differential cross section of $|\eta(\mathrm{b}_{3})|$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $p_{\mathrm{T}}(\mathrm{b}_{3})$ in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space.
Normalized differential cross section of $p_{\mathrm{T}}(\mathrm{b}_{3})$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $|\eta(\mathrm{b}_{4})|$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $p_{\mathrm{T}}(\mathrm{b}_{4})$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $H^{\mathrm{b}}_{\mathrm{T}}$ in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space.
Normalized differential cross section of $H^{\mathrm{b}}_{\mathrm{T}}$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $|\Delta\phi(\mathrm{lj}^{\mathrm{extra}}_{1},\mathrm{b}_{\mathrm{soft}})|$ in $\geq 6$ jets: $\geq 3 \mathrm{b}$, $\geq 3$ light phase space.
Normalized differential cross section of $|\Delta\phi(\mathrm{lj}^{\mathrm{extra}}_{1},\mathrm{b}_{\mathrm{soft}})|$ in $\geq 7$ jets: $\geq 4 \mathrm{b}$, $\geq 3$ light phase space.
Normalized differential cross section of $|\eta(\mathrm{b}^{\mathrm{extra}}_{1})|$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $p_{\mathrm{T}}(\mathrm{b}^{\mathrm{extra}}_{1})$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $|\eta(\mathrm{b}^{\mathrm{extra}}_{2})|$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $p_{\mathrm{T}}(\mathrm{b}^{\mathrm{extra}}_{2})$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $|\eta(\mathrm{b}\mathrm{b}^{\mathrm{extra}})|$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $\Delta\mathrm{R}(\mathrm{b}\mathrm{b}^{\mathrm{extra}})$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $\mathrm{m}(\mathrm{b}\mathrm{b}^{\mathrm{extra}})$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $p_{\mathrm{T}}(\mathrm{b}\mathrm{b}^{\mathrm{extra}})$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $p_{\mathrm{T}}(\mathrm{lj}^{\mathrm{extra}}_{1})$ in $\geq 6$ jets: $\geq 3 \mathrm{b}$, $\geq 3$ light phase space.
Normalized differential cross section of $p_{\mathrm{T}}(\mathrm{lj}^{\mathrm{extra}}_{1})$ in $\geq 7$ jets: $\geq 4 \mathrm{b}$, $\geq 3$ light phase space.
Normalized differential cross section of $H^{\mathrm{j}}_{\mathrm{T}}$ in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space.
Normalized differential cross section of $H^{\mathrm{j}}_{\mathrm{T}}$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $\mathrm{m}_{\mathrm{b}\mathrm{b}}^{\mathrm{max}}$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $H^{\mathrm{light}}_{\mathrm{T}}$ in $\geq 6$ jets: $\geq 3 \mathrm{b}$, $\geq 3$ light phase space.
Normalized differential cross section of $H^{\mathrm{light}}_{\mathrm{T}}$ in $\geq 7$ jets: $\geq 4 \mathrm{b}$, $\geq 3$ light phase space.
Normalized differential cross section of $N_{\mathrm{jets}}$ in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space.
Normalized differential cross section of $N_{\mathrm{jets}}$ in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space.
Normalized differential cross section of $N_{\mathrm{b}}$ in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space.
Correlation of parameters of interest in fit of $|\eta(\mathrm{b}^{\mathrm{add.}}_{1})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $p_{\mathrm{T}}(\mathrm{b}^{\mathrm{add.}}_{1})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $|\eta(\mathrm{b}^{\mathrm{add.}}_{2})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $p_{\mathrm{T}}(\mathrm{b}^{\mathrm{add.}}_{2})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $|\eta(\mathrm{b}\mathrm{b}^{\mathrm{add.}})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $\Delta\mathrm{R}(\mathrm{b}\mathrm{b}^{\mathrm{add.}})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $\mathrm{m}(\mathrm{b}\mathrm{b}^{\mathrm{add.}})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $p_{\mathrm{T}}(\mathrm{b}\mathrm{b}^{\mathrm{add.}})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $\Delta\mathrm{R}_{\mathrm{b}\mathrm{b}}^{\mathrm{avg}}$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $|\eta(\mathrm{b}_{3})|$ observable in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $|\eta(\mathrm{b}_{3})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $p_{\mathrm{T}}(\mathrm{b}_{3})$ observable in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $p_{\mathrm{T}}(\mathrm{b}_{3})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $|\eta(\mathrm{b}_{4})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $p_{\mathrm{T}}(\mathrm{b}_{4})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $H^{\mathrm{b}}_{\mathrm{T}}$ observable in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $H^{\mathrm{b}}_{\mathrm{T}}$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $|\Delta\phi(\mathrm{lj}^{\mathrm{extra}}_{1},\mathrm{b}_{\mathrm{soft}})|$ observable in $\geq 6$ jets: $\geq 3 \mathrm{b}$, $\geq 3$ light phase space
Correlation of parameters of interest in fit of $|\Delta\phi(\mathrm{lj}^{\mathrm{extra}}_{1},\mathrm{b}_{\mathrm{soft}})|$ observable in $\geq 7$ jets: $\geq 4 \mathrm{b}$, $\geq 3$ light phase space
Correlation of parameters of interest in fit of $|\eta(\mathrm{b}^{\mathrm{extra}}_{1})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $p_{\mathrm{T}}(\mathrm{b}^{\mathrm{extra}}_{1})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $|\eta(\mathrm{b}^{\mathrm{extra}}_{2})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $p_{\mathrm{T}}(\mathrm{b}^{\mathrm{extra}}_{2})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $|\eta(\mathrm{b}\mathrm{b}^{\mathrm{extra}})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $\Delta\mathrm{R}(\mathrm{b}\mathrm{b}^{\mathrm{extra}})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $\mathrm{m}(\mathrm{b}\mathrm{b}^{\mathrm{extra}})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $p_{\mathrm{T}}(\mathrm{b}\mathrm{b}^{\mathrm{extra}})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $p_{\mathrm{T}}(\mathrm{lj}^{\mathrm{extra}}_{1})$ observable in $\geq 6$ jets: $\geq 3 \mathrm{b}$, $\geq 3$ light phase space
Correlation of parameters of interest in fit of $p_{\mathrm{T}}(\mathrm{lj}^{\mathrm{extra}}_{1})$ observable in $\geq 7$ jets: $\geq 4 \mathrm{b}$, $\geq 3$ light phase space
Correlation of parameters of interest in fit of $H^{\mathrm{j}}_{\mathrm{T}}$ observable in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $H^{\mathrm{j}}_{\mathrm{T}}$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $\mathrm{m}_{\mathrm{b}\mathrm{b}}^{\mathrm{max}}$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $H^{\mathrm{light}}_{\mathrm{T}}$ observable in $\geq 6$ jets: $\geq 3 \mathrm{b}$, $\geq 3$ light phase space
Correlation of parameters of interest in fit of $H^{\mathrm{light}}_{\mathrm{T}}$ observable in $\geq 7$ jets: $\geq 4 \mathrm{b}$, $\geq 3$ light phase space
Correlation of parameters of interest in fit of $N_{\mathrm{jets}}$ observable in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $N_{\mathrm{jets}}$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Correlation of parameters of interest in fit of $N_{\mathrm{b}}$ observable in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $|\eta(\mathrm{b}^{\mathrm{add.}}_{1})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $p_{\mathrm{T}}(\mathrm{b}^{\mathrm{add.}}_{1})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $|\eta(\mathrm{b}^{\mathrm{add.}}_{2})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $p_{\mathrm{T}}(\mathrm{b}^{\mathrm{add.}}_{2})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $|\eta(\mathrm{b}\mathrm{b}^{\mathrm{add.}})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $\Delta\mathrm{R}(\mathrm{b}\mathrm{b}^{\mathrm{add.}})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $\mathrm{m}(\mathrm{b}\mathrm{b}^{\mathrm{add.}})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $p_{\mathrm{T}}(\mathrm{b}\mathrm{b}^{\mathrm{add.}})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $\Delta\mathrm{R}_{\mathrm{b}\mathrm{b}}^{\mathrm{avg}}$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $|\eta(\mathrm{b}_{3})|$ observable in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $|\eta(\mathrm{b}_{3})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $p_{\mathrm{T}}(\mathrm{b}_{3})$ observable in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $p_{\mathrm{T}}(\mathrm{b}_{3})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $|\eta(\mathrm{b}_{4})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $p_{\mathrm{T}}(\mathrm{b}_{4})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $H^{\mathrm{b}}_{\mathrm{T}}$ observable in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $H^{\mathrm{b}}_{\mathrm{T}}$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $|\Delta\phi(\mathrm{lj}^{\mathrm{extra}}_{1},\mathrm{b}_{\mathrm{soft}})|$ observable in $\geq 6$ jets: $\geq 3 \mathrm{b}$, $\geq 3$ light phase space
Covariances of all nuisance parameters and POIs in fit of $|\Delta\phi(\mathrm{lj}^{\mathrm{extra}}_{1},\mathrm{b}_{\mathrm{soft}})|$ observable in $\geq 7$ jets: $\geq 4 \mathrm{b}$, $\geq 3$ light phase space
Covariances of all nuisance parameters and POIs in fit of $|\eta(\mathrm{b}^{\mathrm{extra}}_{1})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $p_{\mathrm{T}}(\mathrm{b}^{\mathrm{extra}}_{1})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $|\eta(\mathrm{b}^{\mathrm{extra}}_{2})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $p_{\mathrm{T}}(\mathrm{b}^{\mathrm{extra}}_{2})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $|\eta(\mathrm{b}\mathrm{b}^{\mathrm{extra}})|$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $\Delta\mathrm{R}(\mathrm{b}\mathrm{b}^{\mathrm{extra}})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $\mathrm{m}(\mathrm{b}\mathrm{b}^{\mathrm{extra}})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $p_{\mathrm{T}}(\mathrm{b}\mathrm{b}^{\mathrm{extra}})$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $p_{\mathrm{T}}(\mathrm{lj}^{\mathrm{extra}}_{1})$ observable in $\geq 6$ jets: $\geq 3 \mathrm{b}$, $\geq 3$ light phase space
Covariances of all nuisance parameters and POIs in fit of $p_{\mathrm{T}}(\mathrm{lj}^{\mathrm{extra}}_{1})$ observable in $\geq 7$ jets: $\geq 4 \mathrm{b}$, $\geq 3$ light phase space
Covariances of all nuisance parameters and POIs in fit of $H^{\mathrm{j}}_{\mathrm{T}}$ observable in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $H^{\mathrm{j}}_{\mathrm{T}}$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $\mathrm{m}_{\mathrm{b}\mathrm{b}}^{\mathrm{max}}$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $H^{\mathrm{light}}_{\mathrm{T}}$ observable in $\geq 6$ jets: $\geq 3 \mathrm{b}$, $\geq 3$ light phase space
Covariances of all nuisance parameters and POIs in fit of $H^{\mathrm{light}}_{\mathrm{T}}$ observable in $\geq 7$ jets: $\geq 4 \mathrm{b}$, $\geq 3$ light phase space
Covariances of all nuisance parameters and POIs in fit of $N_{\mathrm{jets}}$ observable in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $N_{\mathrm{jets}}$ observable in $\geq 6$ jets: $\geq 4 \mathrm{b}$ phase space
Covariances of all nuisance parameters and POIs in fit of $N_{\mathrm{b}}$ observable in $\geq 5$ jets: $\geq 3 \mathrm{b}$ phase space
Fiducial cross sections from the measurements of all observables, compared to predictions from different ttbb simulation approaches. For each of the normalized differential measurements the fiducial cross section in the respective phase space is also determined. In the paper only one representative observable is quoted for each fiducial phase space, while here the measured cross section with the uncertainties from the fit to the respective observable is summarized.
The first evidence for the standard model production of a top quark in association with a W boson and a Z boson is reported. The measurement is performed in multilepton final states, where the Z boson is reconstructed via its decays to electron or muon pairs and the W boson decays either to leptons or hadrons. The analysed data were recorded by the CMS experiment at the CERN LHC in 2016-2018 in proton-proton collisions at $\sqrt{s}$ = 13 TeV, and correspond to an integrated luminosity of 138 fb$^{-1}$. The measured cross section is 354 $\pm$ 54 (stat) $\pm$ 95 (syst) fb, and corresponds to a statistical significance of 3.4 standard deviations.
Expected yields for signal and background processes and observed number of events in the signal and control regions
Postfit b jet multiplicity distribution in the $\text{SR}_\text{4l}$
Postfit score of the tWZ output node from the multiclass classifier in $\text{SR}_\text{3l,3j}$ for events with exactly 1 b jet
Postfit score of the $\text{t}\bar{\text{t}}\text{Z}$ output node from the multiclass classifier in $\text{SR}_\text{3l,3j}$ for events with at least 2 b jets
Postfit score of the tWZ output node from the binary classifier in $\text{SR}_\text{3l,2j}$
$\text{p}_\text{T}$ of the leading jet in the $\text{SR}_\text{3l,2j}$
$\text{p}_\text{T}$ of the leading lepton in the $\text{SR}_\text{3l,2j}$
Max $\text{p}_\text{T}$ of the lepton-jet in the $\text{SR}_\text{3l,3j}$
Invariant mass of the system of leptons, jets, and $\vec{\text{p}}^\text{miss}_\text{T}$ in the $\text{SR}_\text{3l,3j}$
Two-dimensional likelihood scan of the signal strenghts of tWZ ($\mu_\text{tWZ}$) vs. $\text{t}\bar{\text{t}}\text{Z}$ ($\mu_{\text{t}\bar{\text{t}}\text{Z}}$). The blue lines show the 68%, 95%, and 99% confidence level contours. The black cross represents the best-fit value, while the red diamond the SM expectation
Two-dimensional likelihood scan of the signal strenghts of tWZ ($\mu_\text{tWZ}$) vs. $\text{t}\bar{\text{t}}\text{Z}$ ($\mu_{\text{t}\bar{\text{t}}\text{Z}}$). The blue lines show the 68%, 95%, and 99% confidence level contours. The black cross represents the best-fit value, while the red diamond the SM expectation
A search for the production of long-lived particles in proton-proton collisions at a center-of-mass energy of 13 TeV at the CERN LHC is presented. The search is based on data collected by the CMS experiment in 2016-2018, corresponding to a total integrated luminosity of 137 fb$^{-1}$. This search is designed to be sensitive to long-lived particles with mean proper decay lengths between 0.1 and 1000 $\mu$m, whose decay products produce a final state with at least one displaced vertex and missing transverse momentum. A machine learning algorithm, which improves the background rejection power by more than an order of magnitude, is applied to improve the sensitivity. The observation is consistent with the standard model background prediction, and the results are used to constrain split supersymmetry (SUSY) and gauge-mediated SUSY breaking models with different gluino mean proper decay lengths and masses. This search is the first CMS search that shows sensitivity to hadronically decaying long-lived particles from signals with mass differences between the gluino and neutralino below 100 GeV. It sets the most stringent limits to date for split-SUSY models and gauge-mediated SUSY breaking models with gluino proper decay length less than 6 $\mu$m.
Distributions of $S_{\mathrm{ML}}$ for data, simulated background and signal events with $n_{\mathrm{track}}$ of 3. The distributions are shown for split-SUSY signals with a gluino mass of 2000 GeV and neutralino mass of 1900 GeV. Different gluino proper decay lengths are shown as $c\tau$ in the legend. All distributions are normalized to unity.
Distributions of $S_{\mathrm{ML}}$ for data, simulated background and signal events with $n_{\mathrm{track}}$ of 3. The distributions are shown for split-SUSY signals with a gluino mass of 2000 GeV and neutralino mass of 1800 GeV. Different gluino proper decay lengths are shown as $c\tau$ in the legend. All distributions are normalized to unity.
Distributions of $S_{\mathrm{ML}}$ for data, simulated background and signal events with $n_{\mathrm{track}}$ of 4. The distributions are shown for split-SUSY signals with a gluino mass of 2000 GeV and neutralino mass of 1900 GeV. Different gluino proper decay lengths are shown as $c\tau$ in the legend. All distributions are normalized to unity.
Distributions of $S_{\mathrm{ML}}$ for data, simulated background and signal events with $n_{\mathrm{track}}$ of 4. The distributions are shown for split-SUSY signals with a gluino mass of 2000 GeV and neutralino mass of 1800 GeV. Different gluino proper decay lengths are shown as $c\tau$ in the legend. All distributions are normalized to unity.
Distributions of $S_{\mathrm{ML}}$ for data, simulated background and signal events with $n_{\mathrm{track}}$ of $\geq$ 5. The distributions are shown for split-SUSY signals with a gluino mass of 2000 GeV and neutralino mass of 1900 GeV. Different gluino proper decay lengths are shown as $c\tau$ in the legend. All distributions are normalized to unity.
Distributions of $S_{\mathrm{ML}}$ for data, simulated background and signal events with $n_{\mathrm{track}}$ of $\geq$ 5. The distributions are shown for split-SUSY signals with a gluino mass of 2000 GeV and neutralino mass of 1800 GeV. Different gluino proper decay lengths are shown as $c\tau$ in the legend. All distributions are normalized to unity.
The distribution of $n_{\mathrm{track}}$ in different $S_{\mathrm{ML}}$ regions for simulated background events. Events with 0 $ < S_{\mathrm{ML}} < $ 0.2 (blue), 0.2 $ < S_{\mathrm{ML}} < $ 0.6 (red), and 0.6 $ < S_{\mathrm{ML}} < $ 1.0 (green) are compared. All distributions are normalized to unity. The similar $n_{\mathrm{track}}$ distributions demonstrate that $n_{\mathrm{track}}$ and $S_{\mathrm{ML}}$ are decorrelated.
The distribution of $d_{\mathrm{BV}}$ in $K_{\mathrm{S}}^{\mathrm{0}}$ vertices in data (black) and simulation (purple). The lower panel shows the ratio between data and simulation.
The vertex reconstruction efficiency for artificially displaced vertices in data (black) and simulation (red). In this example, the artificially displaced vertices are corrected to mimic split-SUSY signal events with gluino mass of 2000 GeV and neutralino mass of 1800 GeV.
The ML tagging efficiency for artificially displaced vertices in data (black) and simulation (red). In this example, the artificially displaced vertices are corrected to mimic split-SUSY signal events with gluino mass of 2000 GeV and neutralino mass of 1800 GeV.
Number of predicted and observed events in the control, validation, and search regions. Predictions are calculated using Eqs. (2) and (3) and fitting the data under the background-only hypothesis. Regions are organized by $S_{\mathrm{ML}}$ and $n_{\mathrm{track}}$ values, and region names corresponding with Fig. 7 are given in parentheses. The predicted number of events that pass the $S_{\mathrm{ML}}$ selection and the observed number of events that pass or fail the $S_{\mathrm{ML}}$ selection are shown in seperate rows.
The 95% CL upper limit on the product of the cross section and branching fraction squared for the split-SUSY signal model with a mass splitting of 100 GeV, shown as a function of gluino mass and $c\tau$. The observed (solid black) and expected (dashed red) exclusion curves are overlaid on the limit plot.
The 95% CL upper limit on the product of the cross section and branching fraction squared for the split-SUSY signal model with a mass splitting of 100 GeV, shown as a function of gluino mass and $c\tau$. The observed (solid black) and expected (dashed red) exclusion curves are overlaid on the limit plot.
The 95% CL upper limit on the product of the cross section and branching fraction squared for the split-SUSY model with a $c\tau$ of 10 mm, shown as a function of gluino mass and mass splitting. The observed (solid black) and expected (dashed red) exclusion curves are overlaid on the limit plot.
The 95% CL upper limit on the product of the cross section and branching fraction squared for the split-SUSY model with a $c\tau$ of 10 mm, shown as a function of gluino mass and mass splitting. The observed (solid black) and expected (dashed red) exclusion curves are overlaid on the limit plot.
The 95% CL upper limit on the product of the cross section and branching fraction squared for the GMSB SUSY signal model, shown as a function of gluino mass and $c\tau$. The observed (solid black) and expected (dashed red) exclusion curves are overlaid on the limit plot.
The 95% CL upper limit on the product of the cross section and branching fraction squared for the GMSB SUSY signal model, shown as a function of gluino mass and $c\tau$. The observed (solid black) and expected (dashed red) exclusion curves are overlaid on the limit plot.
A study of the anomalous couplings of the Higgs boson to vector bosons, including $CP$-violation effects, has been conducted using its production and decay in the WW channel. This analysis is performed on proton-proton collision data collected with the CMS detector at the CERN LHC during 2016-2018 at a center-of-mass energy of 13 TeV, and corresponds to an integrated luminosity of 138 fb$^{-1}$. The different-flavor dilepton (e$\mu$) final state is analyzed, with dedicated categories targeting gluon fusion, electroweak vector boson fusion, and associated production with a W or Z boson. Kinematic information from associated jets is combined using matrix element techniques to increase the sensitivity to anomalous effects at the production vertex. A simultaneous measurement of four Higgs boson couplings to electroweak vector bosons is performed in the framework of a standard model effective field theory. All measurements are consistent with the expectations for the standard model Higgs boson and constraints are set on the fractional contribution of the anomalous couplings to the Higgs boson production cross section.
Expected profiled likelihood on $f_{a2}$ using Approach 1. The signal strength modifiers are treated as free parameters. Axis scales are varied to improve the visibility of important features.
Observed profiled likelihood on $f_{a2}$ using Approach 1. The signal strength modifiers are treated as free parameters. Axis scales are varied to improve the visibility of important features.
Expected profiled likelihood on $f_{\Lambda1}$ using Approach 1. The signal strength modifiers are treated as free parameters. Axis scales are varied to improve the visibility of important features.
Observed profiled likelihood on $f_{\Lambda1}$ using Approach 1. The signal strength modifiers are treated as free parameters. Axis scales are varied to improve the visibility of important features.
Expected profiled likelihood on $f_{a3}$ using Approach 1. The signal strength modifiers are treated as free parameters.
Observed profiled likelihood on $f_{a3}$ using Approach 1. The signal strength modifiers are treated as free parameters.
Expected profiled likelihood on $f_{\Lambda1}^{Z\gamma}$ using Approach 1. The signal strength modifiers are treated as free parameters.
Observed profiled likelihood on $f_{\Lambda1}^{Z\gamma}$ using Approach 1. The signal strength modifiers are treated as free parameters.
Expected profiled likelihood on $f_{a2}$ using Approach 2. The other two anomalous coupling cross section fractions are fixed to zero. The signal strength modifiers are treated as free parameters. Axis scales are varied to improve the visibility of important features.
Observed profiled likelihood on $f_{a2}$ using Approach 2. The other two anomalous coupling cross section fractions are fixed to zero. The signal strength modifiers are treated as free parameters. Axis scales are varied to improve the visibility of important features.
Expected profiled likelihood on $f_{\Lambda1}$ using Approach 2. The other two anomalous coupling cross section fractions are fixed to zero. The signal strength modifiers are treated as free parameters. Axis scales are varied to improve the visibility of important features.
Observed profiled likelihood on $f_{\Lambda1}$ using Approach 2. The other two anomalous coupling cross section fractions are fixed to zero. The signal strength modifiers are treated as free parameters. Axis scales are varied to improve the visibility of important features.
Expected profiled likelihood on $f_{a3}$ using Approach 2. The other two anomalous coupling cross section fractions are fixed to zero. The signal strength modifiers are treated as free parameters.
Observed profiled likelihood on $f_{a3}$ using Approach 2. The other two anomalous coupling cross section fractions are fixed to zero. The signal strength modifiers are treated as free parameters.
Expected profiled likelihood on $f_{a2}$ using Approach 2. The other two anomalous coupling cross section fractions are left floating in the fit. The signal strength modifiers are treated as free parameters. Axis scales are varied to improve the visibility of important features.
Observed profiled likelihood on $f_{a2}$ using Approach 2. The other two anomalous coupling cross section fractions are left floating in the fit. The signal strength modifiers are treated as free parameters. Axis scales are varied to improve the visibility of important features.
Expected profiled likelihood on $f_{\Lambda1}$ using Approach 2. The other two anomalous coupling cross section fractions are left floating in the fit. The signal strength modifiers are treated as free parameters. Axis scales are varied to improve the visibility of important features.
Observed profiled likelihood on $f_{\Lambda1}$ using Approach 2. The other two anomalous coupling cross section fractions are left floating in the fit. The signal strength modifiers are treated as free parameters. Axis scales are varied to improve the visibility of important features.
Expected profiled likelihood on $f_{a3}$ using Approach 2. The other two anomalous coupling cross section fractions are left floating in the fit. The signal strength modifiers are treated as free parameters.
Observed profiled likelihood on $f_{a3}$ using Approach 2. The other two anomalous coupling cross section fractions are left floating in the fit. The signal strength modifiers are treated as free parameters.
Expected profiled likelihood on the $\delta c_{Z}$ coupling of the SMEFT Higgs basis.
Observed profiled likelihood on the $\delta c_{Z}$ coupling of the SMEFT Higgs basis.
Expected profiled likelihood on the $c_{Z\Box}$ coupling of the SMEFT Higgs basis.
Observed profiled likelihood on the $c_{Z\Box}$ coupling of the SMEFT Higgs basis.
Expected profiled likelihood on the $c_{ZZ}$ coupling of the SMEFT Higgs basis.
Observed profiled likelihood on the $c_{ZZ}$ coupling of the SMEFT Higgs basis.
Expected profiled likelihood on the $\tilde{c}_{ZZ}$ coupling of the SMEFT Higgs basis.
Observed profiled likelihood on the $\tilde{c}_{ZZ}$ coupling of the SMEFT Higgs basis.
Expected profiled likelihood on $f_{a3}^{ggH}$. The signal strength modifiers and the CP-odd HVV anomalous coupling cross section fraction are treated as free parameters.
Observed profiled likelihood on $f_{a3}^{ggH}$. The signal strength modifiers and the CP-odd HVV anomalous coupling cross section fraction are treated as free parameters.
A search for long-lived heavy neutrinos (N) in the decays of \PB mesons produced in proton-proton collisions at $\sqrt{s}$ = 13 TeV is presented. The data sample corresponds to an integrated luminosity of 41.6 fb$^{-1}$ collected in 2018 by the CMS experiment at the CERN LHC, using a dedicated data stream that enhances the number of recorded events containing B mesons. The search probes heavy neutrinos with masses in the range 1 $\lt$$m_\mathrm{N}$$\lt$ 3 GeV and decay lengths in the range 10$^{-2}$$\lt$$c\tau$$\lt$ 10$^{4}$ mm, where $\tau_\mathrm{N}$ is the N proper mean lifetime. Signal events are defined by the signature B $\to$$\ell_\mathrm{B}$NX; N $\to$$\ell^{\pm} \pi^{\mp}$, where the leptons $\ell_\mathrm{B}$ and $\ell$ can be either a muon or an electron, provided that at least one of them is a muon. The hadronic recoil system, X, is treated inclusively and is not reconstructed. No significant excess of events over the standard model background is observed in any of the $\ell^{\pm}\pi^{\mp}$ invariant mass distributions. Limits at 95% confidence level on the sum of the squares of the mixing amplitudes between heavy and light neutrinos, $\vert V_\mathrm{N}\vert^2$, and on $c\tau$ are obtained in different mixing scenarios for both Majorana and Dirac-like N particles. The most stringent upper limit $\vert V_\mathrm{N}\vert^2$ $\lt$ 2.0$\times$10$^{-5}$ is obtained at $m_\mathrm{N}$ = 1.95 GeV for the Majorana case where N mixes exclusively with muon neutrinos. The limits on $\vert V_\mathrm{N}\vert^2$ for masses 1 $\lt$ $m_\mathrm{N}$ $\lt$ 1.7 GeV are the most stringent from a collider experiment to date.
Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.0, 1.0, 0.0) and in the Majorana scenario.
Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.0, 0.5, 0.5) and in the Majorana scenario.
Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.5, 0.5, 0.0) and in the Majorana scenario.
Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.33, 0.33, 0.33) and in the Majorana scenario.
Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.0, 1.0, 0.0) and in the Dirac-like scenario.
Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.0, 0.5, 0.5) and in the Dirac-like scenario.
Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.5, 0.5, 0.0) and in the Dirac-like scenario.
Expected and observed 95% CL upper limits on $|V_\mathrm{N}|^2$ as a function of $m_\mathrm{N}$ for the mixing scenario ($r_e$, $r_\mu$, $r_\tau$) = (0.33, 0.33, 0.33) and in the Dirac-like scenario.
Observed 95% CL lower limits on $c\tau_\mathrm{N}$ as functions of the mixing ratios ($r_e$, $r_\mu$, $r_\tau$) for a fixed N mass of 1.0 GeV in the Majorana scenario.
Observed 95% CL lower limits on $c\tau_\mathrm{N}$ as functions of the mixing ratios ($r_e$, $r_\mu$, $r_\tau$) for a fixed N mass of 1.5 GeV in the Majorana scenario.
Observed 95% CL lower limits on $c\tau_\mathrm{N}$ as functions of the mixing ratios ($r_e$, $r_\mu$, $r_\tau$) for a fixed N mass of 2.0 GeV in the Majorana scenario.
Observed 95% CL lower limits on $c\tau_\mathrm{N}$ as functions of the mixing ratios ($r_e$, $r_\mu$, $r_\tau$) for a fixed N mass of 1.0 GeV in the Dirac-like scenario.
Observed 95% CL lower limits on $c\tau_\mathrm{N}$ as functions of the mixing ratios ($r_e$, $r_\mu$, $r_\tau$) for a fixed N mass of 1.5 GeV in the Dirac-like scenario.
Observed 95% CL lower limits on $c\tau_\mathrm{N}$ as functions of the mixing ratios ($r_e$, $r_\mu$, $r_\tau$) for a fixed N mass of 2.0 GeV in the Dirac-like scenario.
A search for exotic decays of the Higgs boson (H) with a mass of 125 GeV to a pair of light pseudoscalars $\mathrm{a}_1$ is performed in final states where one pseudoscalar decays to two b quarks and the other to a pair of muons or $\tau$ leptons. A data sample of proton-proton collisions at $\sqrt{s}$ = 13 TeV corresponding to an integrated luminosity of 138 fb$^{-1}$ recorded with the CMS detector is analyzed. No statistically significant excess is observed over the standard model backgrounds. Upper limits are set at 95% confidence level (CL) on the Higgs boson branching fraction to $\mu\mu$bb and to $\tau\tau$bb, via a pair of $\mathrm{a}_1$s. The limits depend on the pseudoscalar mass $m_{\mathrm{a}_1}$ and are observed to be in the range (0.17-3.3) $\times$ 10$^{-4}$ and (1.7-7.7) $\times$ 10$^{2}$ in the $\mu\mu$bb and $\tau\tau$bb final states, respectively. In the framework of models with two Higgs doublets and a complex scalar singlet (2HDM+S), the results of the two final states are combined to determine model-independent upper limits on the branching fraction $\mathcal{B}$(H $\to$ $\mathrm{a}_1\mathrm{a}_1$ $\to$ $\ell\ell$bb) at 95% CL, with $\ell$ being a muon or a $\tau$ lepton. For different types of 2HDM+S, upper bounds on the branching fraction $\mathcal{B}$(H $\to$ $\mathrm{a}_1\mathrm{a}_1$) are extracted from the combination of the two channels. In most of the Type II 2HDM+S parameter space, $\mathcal{B}($H $\to$ $\mathrm{a}_1\mathrm{a}_1$) values above 0.23 are excluded at 95% CL for $m_{\mathrm{a}_1}$ values between 15 and 60 GeV.
Observed and expected upper limits at 95% CL on B($\text{H} \rightarrow \text{a}_{1}\text{a}_{1} \rightarrow \mu\mu$bb) as functions of $m_{\text{a}_{1}}$. The inner and outer bands indicate the regions containing the distribution of limits located within 68 and 95% confidence intervals, respectively, of the expectation under the background-only hypothesis.
Observed and expected upper limits at 95% CL on B($\text{H} \rightarrow \text{a}_{1}\text{a}_{1} \rightarrow \tau\tau$bb) in percent as functions of $m_{\text{a}_{1}}$, for the combination of the $\mu\tau_{\text{h}}$, $e\tau_{\text{h}}$, and $e\mu$ channels. The inner and outer bands indicate the regions containing the distribution of limits located within 68 and 95% confidence intervals, respectively, of the expectation under the background-only hypothesis.
Observed and expected upper limits at 95% CL on B($\text{H} \rightarrow \text{a}_{1}\text{a}_{1} \rightarrow ll$bb) in percent, where $l$ stands for muons or $\tau$ leptons, obtained from the combination of the $\mu\mu$bb and $\tau\tau$bb channels. The results are obtained as functions $m_{\text{a}_{1}}$ for 2HDM+S models, independent of the type and tan $\beta$ parameter. The inner and outer bands indicate the regions containing the distribution of limits located within 68 and 95% confidence intervals, respectively, of the expectation under the background-only hypothesis.
Observed upper limits at 95% CL on B($\text{H} \rightarrow \text{a}_{1}\text{a}_{1}$) in percent, obtained from the combination of the $\mu\mu$bb and $\tau\tau$bb channels. The results are obtained as functions of $m_{\text{a}_{1}}$ for 2HDM+S Type I (independent of tan$\beta$), Type II (tan$\beta$=2.0), Type III (tan$\beta$=2.0), and Type IV (tan$\beta$=0.6), respectively.
A search is presented for baryon number violating interactions in top quark production and decay. The analysis uses data from proton-proton collisions at a center-of-mass energy of 13 TeV, collected with the CMS detector at the LHC with an integrated luminosity of 138 fb$^{-1}$. Candidate events are selected by requiring two oppositely-charged leptons (electrons or muons) and exactly one jet identified as originating from a bottom quark. Multivariate discriminants are used to separate the signal from the background. No significant deviation from the standard model prediction is observed. Upper limits are placed on the strength of baryon number violating couplings. For the first time the production of single top quarks via baryon number violating interactions is studied. This allows the search to set the most stringent constraints to date on the branching fraction of the top quark decay to a lepton, an up-type quark (u or c), and a down-type quark (d, s, or b). The results improve the previous bounds by three to six orders of magnitude based on the fermion flavor combination of the baryon number violating interactions.
The observed upper limits on the branching fractions of the top quark BNV decays are shown with circle and triangle shapes for electron and muon couplings, respectively. The observed limits corresponding to the $C_t$ and $C_s$ coefficients are shown with filled and open markers, respectively. The yellow light (green dark) bands indicate the range within plus or minus one (two) standard deviations bands around the expected limits.
Energy correlators that describe energy-weighted distances between two or three particles in a jet are measured using an event sample of $\sqrt{s}$ = 13 TeV proton-proton collisions collected by the CMS experiment and corresponding to an integrated luminosity of 36.3 fb$^{-1}$. The measured distributions reveal two key features of the strong interaction: confinement and asymptotic freedom. By comparing the ratio of the two measured distributions with theoretical calculations that resum collinear emissions at approximate next-to-next-to-leading logarithmic accuracy matched to a next-to-leading order calculation, the strong coupling is determined at the Z boson mass: $\alpha_\mathrm{S}(m_\mathrm{Z})$ = 0.1229$^{+0.0040}_{-0.0050}$, the most precise $\alpha_\mathrm{S}(m_\mathrm{Z})$ value obtained using jet substructure observables.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E2C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
Unfolded E3C/E2C distributions in data compared to NLO+NNLL_approx predictions. Theoretial uncertainty in each bin is handled fully correlated as shape uncertainty. For the one-sided uncertainties, we symmetrize them when performing the fit.
The fitted slopes of the E3C/E2C data distributions as a function of jet pt are used to illustrate the dependency of alphas on jet pt.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
Unfolded E3C/E2C distributions in data compared to MC predictions.
The chi2 scan result using eq.3 for different alphas.
The correlation matrix is composed by 10 jet pt region, each region is represented by a block in the plot. Inside each block, there are 22 xL bins same as the E2C, E3C and E3C/E2C distributions. Therefore, the x and y bins of the correlation matrix is given by, binNumber = pT_index * 22 + xL_index.
The correlation matrix is composed by 10 jet pt region, each region is represented by a block in the plot. Inside each block, there are 22 xL bins same as the E2C, E3C and E3C/E2C distributions. Therefore, the x and y bins of the correlation matrix is given by, binNumber = pT_index * 22 + xL_index.
The correlation matrix is composed by 10 jet pt region, each region is represented by a block in the plot. Inside each block, there are 22 xL bins same as the E2C, E3C and E3C/E2C distributions. Therefore, the x and y bins of the correlation matrix is given by, binNumber = pT_index * 22 + xL_index.
The energy weight of E2C as defined in eq.1 in the paper is used in the unfolding, the binning is listed in this table.
The energy weight of E3C as defined in eq.1 in the paper is used in the unfolding, the binning is listed in this table.
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