Showing 10 of 20 results
We report first results from an analysis based on a new multi-hadron correlation technique, exploring jet-medium interactions and di-jet surface emission bias at RHIC. Pairs of back-to-back high transverse momentum hadrons are used for triggers to study associated hadron distributions. In contrast with two- and three-particle correlations with a single trigger with similar kinematic selections, the associated hadron distribution of both trigger sides reveals no modification in either relative pseudo-rapidity or relative azimuthal angle from d+Au to central Au+Au collisions. We determine associated hadron yields and spectra as well as production rates for such correlated back-to-back triggers to gain additional insights on medium properties.
Relative production rates for jets and di-jets in Au+Au collisions of different centralities with respect to d+Au data.
Conditional di-jet survival probability in Au+Au data compared to d+Au reference.
Conditional di-jet survival probability in Au+Au data compared to d+Au reference.
We present the measurement of non-photonic electron production at high transverse momentum ($p_T > $ 2.5 GeV/$c$) in $p$ + $p$ collisions at $\sqrt{s}$ = 200 GeV using data recorded during 2005 and 2008 by the STAR experiment at the Relativistic Heavy Ion Collider (RHIC). The measured cross-sections from the two runs are consistent with each other despite a large difference in photonic background levels due to different detector configurations. We compare the measured non-photonic electron cross-sections with previously published RHIC data and pQCD calculations. Using the relative contributions of B and D mesons to non-photonic electrons, we determine the integrated cross sections of electrons ($\frac{e^++e^-}{2}$) at 3 GeV/$c < p_T <~$10 GeV/$c$ from bottom and charm meson decays to be ${d\sigma_{(B\to e)+(B\to D \to e)} \over dy_e}|_{y_e=0}$ = 4.0$\pm0.5$({\rm stat.})$\pm1.1$({\rm syst.}) nb and ${d\sigma_{D\to e} \over dy_e}|_{y_e=0}$ = 6.2$\pm0.7$({\rm stat.})$\pm1.5$({\rm syst.}) nb, respectively.
Ratio of photon $p_T$ spectra from Fig. 7(a) to inclusive photons $p_T$ spectrum.
Ratio of non-photonic to photonic electron yield from the Run2008 analysis.
Ratio of non-photonic to photonic electron yield from the Run2005 analysis.
Invariant cross section for electrons $(e^+ + e^-)/2$ from bottom meson decay, together with the ratio of the measurements to the FONLL predictions.
Invariant cross section for electrons $(e^+ + e^-)/2$ from charm meson decay, together with the ratio of the measurements to the FONLL predictions.
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. ...
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
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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 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
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raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
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raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
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raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
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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
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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
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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
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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
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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 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 1
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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 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
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raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
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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
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raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
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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
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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 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
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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 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 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 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 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 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 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 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 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 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 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 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 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 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 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
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 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 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 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 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
The contribution of $B$ meson decays to non-photonic electrons, which are mainly produced by the semi-leptonic decays of heavy flavor mesons, in $p+p$ collisions at $\sqrt{s} =$ 200 GeV has been measured using azimuthal correlations between non-photonic electrons and hadrons. The extracted $B$ decay contribution is approximately 50% at a transverse momentum of $p_{T} \geq 5$ GeV/$c$. These measurements constrain the nuclear modification factor for electrons from $B$ and $D$ meson decays. The result indicates that $B$ meson production in heavy ion collisions is also suppressed at high $p_{T}$.
(a) Background-subtracted invariant mass distribution of $K$ pairs requiring at least one nonphotonic electron trigger in the event. The solid line is a Gaussian fit to the data near the peak region. (b) Distribution of the azimuthal angle between nonphotonic electron (positron) trigger particles and $D^{0}$ ($\bar{D}^{0}$). The solid (dashed) line is a fit of the correlation function from PYTHIA (MC$@$NLO) simulations to the data points.
Transverse momentum dependence of the relative contribution from $B$ mesons ($r_{B}$) to the nonphotonic electron yields. Error bars are statistical and brackets are systematic uncertainties. The solid curve is the FONLL calculation [14]. Theoretical uncertainties are indicated by the dashed curves.
We report transverse momentum ($p_{T} \leq15$ GeV/$c$) spectra of $\pi^{\pm}$, $K^{\pm}$, $p$, $\bar{p}$, $K_{S}^{0}$, and $\rho^{0}$ at mid-rapidity in p+p and Au+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV. Perturbative QCD calculations are consistent with $\pi^{\pm}$ spectra in p+p collisions but do not reproduce $K$ and $p(\bar{p})$ spectra. The observed decreasing antiparticle-to-particle ratios with increasing $p_T$ provide experimental evidence for varying quark and gluon jet contributions to high-$p_T$ hadron yields. The relative hadron abundances in Au+Au at $p_{T}{}^{>}_{\sim}8$ GeV/$c$ are measured to be similar to the p+p results, despite the expected Casimir effect for parton energy loss.
The invariant yields $d^2N/(2\pi p_T dp_T dy)$ of $\pi^{\pm}$, $K^{\pm}$, $p$, and $\bar{p}$ from non-singly diffractive p+p collisions ($\sigma_{NSD} = 30.0 \pm 3.5$ mb), and NLO calculations with AKK [9] and DSS [10] FF. The uncertainty of yields due to the scale dependence as evaluated in [10] is about a factor of 2. Bars and boxes (bands) represent statistical and systematic uncertainties, respectively.
The invariant yields $d^2N/(2\pi p_T dp_T dy)$ of $K^0_S$ from non-singly diffractive p+p collisions ($\sigma_{NSD} = 30.0 \pm 3.5$ mb), and NLO calculations with AKK [9] and DSS [10] FF. The uncertainty of yields due to the scale dependence as evaluated in [10] is about a factor of 2. Bars and boxes (bands) represent statistical and systematic uncertainties, respectively.
The invariant yields $d^2N/(2\pi p_T dp_T dy)$ of $\rho^0$ from non-singly diffractive p+p collisions ($\sigma_{NSD} = 30.0 \pm 3.5$ mb), and NLO calculations with AKK [9] and DSS [10] FF. The uncertainty of yields due to the scale dependence as evaluated in [10] is about a factor of 2. Bars and boxes (bands) represent statistical and systematic uncertainties, respectively.
The invariant yields $d^2N/(2\pi p_T dp_T dy)$ of $K + p(\bar{p})$ in central Au+Au collisions, and NLO calculations with AKK [9] and DSS [10] FF. The uncertainty of yields due to the scale dependence as evaluated in [10] is about a factor of 2. Bars and boxes (bands) represent statistical and systematic uncertainties, respectively.
The invariant yields $d^2N/(2\pi p_T dp_T dy)$ of $\rho^0$ in central Au+Au collisions, and NLO calculations with AKK [9] and DSS [10] FF. The uncertainty of yields due to the scale dependence as evaluated in [10] is about a factor of 2. Bars and boxes (bands) represent statistical and systematic uncertainties, respectively.
The invariant yields $d^2N/(2\pi p_T dp_T dy)$ of $K^0_S$ in central Au+Au collisions, and NLO calculations with AKK [9] and DSS [10] FF. The uncertainty of yields due to the scale dependence as evaluated in [10] is about a factor of 2. Bars and boxes (bands) represent statistical and systematic uncertainties, respectively.
Yield ratios $\pi^−/\pi^+$, $\bar{p}/p$, $K^−/K^+$, $p/\pi^+$, $\bar{p}/\pi^−$, and $K^{\pm}/\pi^{\pm}$ versus $p_T$ in p+p collisions, and nominal NLO calculations with AKK [9] and DSS [10] FFs without theoretical uncertainties. Bars and boxes (bands) represent statistical and systematic uncertainties, respectively.
Yield ratio $K^0_S$)/$\pi^{\pm}$ versus $p_T$ in p+p collisions, and nominal NLO calculations with AKK [9] and DSS [10] FFs without theoretical uncertainties. Bars and boxes (bands) represent statistical and systematic uncertainties, respectively.
Yield ratios $p/\pi^+$ and $\bar{p}/\pi^−$ versus $p_T$ in central Au+Au collisions [14] with updated uncertainties at high $p_T$. Bars and boxes (bands) represent statistical and systematic uncertainties, respectively.
$R_{AA}$ of $\pi^{\pm} in central Au+Au collisions as a function of $p_T$. Bars and boxes (bands) represent statistical and systematic uncertainties, respectively. The height of the band at unity represents the normalization uncertainty.
$R_{AA}$ of $K^{\pm}+p(\bar{p})$ in central Au+Au collisions as a function of $p_T$. Bars and boxes (bands) represent statistical and systematic uncertainties, respectively. The height of the band at unity represents the normalization uncertainty.
$R_{AA}$ of $K^0_S$ in central Au+Au collisions as a function of $p_T$. The curves are the calculations for $K^0_S$ $R_{AA}$ with and without jet conversion in medium [15]. Bars and boxes (bands) represent statistical and systematic uncertainties, respectively. The height of the band at unity represents the normalization uncertainty.
$R_{AA}$ of $\rho^0$ in central Au+Au collisions as a function of $p_T$. Bars and boxes (bands) represent statistical and systematic uncertainties, respectively. The height of the band at unity represents the normalization uncertainty.
The ratios of $R_{AA}[K^{\pm} + p(\bar{p})]$ to $R_{AA}(\pi^{\pm})$. The boxes and shaded bands represent the systematic uncertainties for $R_{AA}[K^{\pm} +p(\bar{p})]/R_{AA}(\pi^{\pm})$, respectively.
The ratios of $R_{AA}(K^− + \bar{p})$ to $R_{AA}(K^+ p)$. The systematic uncertainties for $R_{AA}(K^− + \bar{p})/R_{AA}(K^+ +p)$ are 2–12% and left off for clarity.
The ratios of $R_{AA}[\rho^0]$ to $R_{AA}(\pi^{\pm})$. The boxes and shaded bands represent the systematic uncertainties for $R_{AA}(\rho^0)/R_{AA}(\pi^{\pm})$, respectively.
We present first measurements of the evolution of the differential transverse momentum correlation function, {\it C}, with collision centrality in Au+Au interactions at $\sqrt{s_{NN}} = 200$ GeV. {\it C} exhibits a strong dependence on collision centrality that is qualitatively similar to that of number correlations previously reported. We use the observed longitudinal broadening of the near-side peak of {\it C} with increasing centrality to estimate the ratio of the shear viscosity to entropy density, $\eta/s$, of the matter formed in central Au+Au interactions. We obtain an upper limit estimate of $\eta/s$ that suggests that the produced medium has a small viscosity per unit entropy.
The correlation function C, C is plotted in units of (GeV/c)$^2$ and the relative azimuthal angle ∆φ in radians for 70-80% centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Relative statistical errors range from 0.8% in peripheral collisions to 0.9% in the most central collisions at the peak of the distribution.
The correlation function C, C is plotted in units of (GeV/c)$^2$ and the relative azimuthal angle ∆φ in radians for 70-80% centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Relative statistical errors range from 0.8% in peripheral collisions to 0.9% in the most central collisions at the peak of the distribution.
The correlation function C, C is plotted in units of (GeV/c)$^2$ and the relative azimuthal angle ∆φ in radians for 30-40% centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Relative statistical errors range from 0.8% in peripheral collisions to 0.9% in the most central collisions at the peak of the distribution.
The correlation function C, C is plotted in units of (GeV/c)$^2$ and the relative azimuthal angle ∆φ in radians for 30-40% centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Relative statistical errors range from 0.8% in peripheral collisions to 0.9% in the most central collisions at the peak of the distribution.
The correlation function C, C is plotted in units of (GeV/c)$^2$ and the relative azimuthal angle ∆φ in radians for 0-5% centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV..Relative statistical errors range from 0.8% in peripheral collisions to 0.9% in the most central collisions at the peak of the distribution.
The correlation function C, C is plotted in units of (GeV/c)$^2$ and the relative azimuthal angle ∆φ in radians for 0-5% centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV..Relative statistical errors range from 0.8% in peripheral collisions to 0.9% in the most central collisions at the peak of the distribution.
Projection of the correlation function C, for|∆φ|<1.0 radians on the ∆η axis for 70-80% centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The correlation function C is plottedin units of (GeV/c)$^2$.The correlation function C is plotted in units of (GeV/c)$^2$. The solid line shows the fit obtained with Eq.2. The dotted line corresponds to the baseline, b, obtained in the fit and shaded band shows uncertainty in determining b.
Projection of the correlation function C, for|∆φ|<1.0 radians on the ∆η axis for 70-80% centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The correlation function C is plottedin units of (GeV/c)$^2$.The correlation function C is plotted in units of (GeV/c)$^2$. The solid line shows the fit obtained with Eq.2. The dotted line corresponds to the baseline, b, obtained in the fit and shaded band shows uncertainty in determining b.
Projection of the correlation function C, for|∆φ|<1.0 radians on the ∆η axis for 30-40% centrality. Statistical errors at(\Deltaeta_1,Deltaeta_2~(0,0) are approximately 0.084 for Au+Au. The correlation function C is plotted in units of (GeV/c)$^2$. The dotted line corresponds to the baseline,b, obtained in the fit and shaded band shows uncertainty in determining b.
Projection of the correlation function C, for|∆φ|<1.0 radians on the ∆η axis for 30-40% centrality. Statistical errors at(\Deltaeta_1,Deltaeta_2~(0,0) are approximately 0.084 for Au+Au. The correlation function C is plotted in units of (GeV/c)$^2$. The dotted line corresponds to the baseline,b, obtained in the fit and shaded band shows uncertainty in determining b.
Projection of the correlation function C, for|∆φ|<1.0 radians on the ∆η axis for 0-5% centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The correlation functionCis plotted in units of (GeV/c)$^2$. The correlation function C is plotted in units of (GeV/c)$^2$. The solid line shows the fit obtained with Eq.2. The dotted line corresponds to the baseline,b, obtained in the fit and shaded band shows uncertainty in determining b.
Projection of the correlation function C, for|∆φ|<1.0 radians on the ∆η axis for 0-5% centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The correlation functionCis plotted in units of (GeV/c)$^2$. The correlation function C is plotted in units of (GeV/c)$^2$. The solid line shows the fit obtained with Eq.2. The dotted line corresponds to the baseline,b, obtained in the fit and shaded band shows uncertainty in determining b.
We present two-dimensional (2D) two-particle angular correlations on relative pseudorapidity $\eta$ and azimuth $\phi$ for charged particles from Au-Au collisions at $\sqrt{s_{\rm NN}} = 62$ and 200 GeV with transverse momentum $p_t \geq 0.15$ GeV/$c$, $|\eta| \leq 1$ and $2\pi$ azimuth. Observed correlations include a {same-side} (relative azimuth $< \pi/2$) 2D peak, a closely-related away-side azimuth dipole, and an azimuth quadrupole conventionally associated with elliptic flow. The same-side 2D peak and away-side dipole are explained by semihard parton scattering and fragmentation (minijets) in proton-proton and peripheral nucleus-nucleus collisions. Those structures follow N-N binary-collision scaling in Au-Au collisions until mid-centrality where a transition to a qualitatively different centrality trend occurs within a small centrality interval. Above the transition point the number of same-side and away-side correlated pairs increases rapidly {relative to} binary-collision scaling, the $\eta$ width of the same-side 2D peak also increases rapidly ($\eta$ elongation) and the $\phi$ width actually decreases significantly. Those centrality trends are more remarkable when contrasted with expectations of jet quenching in a dense medium. Observed centrality trends are compared to {\sc hijing} predictions and to the expected trends for semihard parton scattering and fragmentation in a thermalized opaque medium. We are unable to reconcile a semihard parton scattering and fragmentation origin for the observed correlation structure and centrality trends with heavy ion collision scenarios which invoke rapid parton thermalization. On the other hand, if the collision system is effectively opaque to few-GeV partons the observations reported here would be inconsistent with a minijet picture.
FIG. 1. (Color online) Perspective views of $2 \mathrm{D}$ charge-independent angular correlations $\Delta \rho / \sqrt{\rho_{\mathrm{ref}}}$ on $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ for Au-Au collisions at $\sqrt{s_{N N}}=200$ and $62 \mathrm{GeV}$ (top and bottom rows, respectively). Centrality increases left to right from most peripheral to most central. Corrected total cross-section fractions are (left to right) $84 \%-93 \%, 55 \%-64 \%, 18 \%-28 \%,$ and $0 \%-5 \%$ for the $200-\mathrm{GeV}$ data and $84 \%-95 \%, 56 \%-65 \%$ $18 \%-28 \%,$ and $0 \%-5 \%$ for the $62 \mathrm{GeV}$ data (see Tables III and IV).
FIG. 1. (Color online) Perspective views of $2 \mathrm{D}$ charge-independent angular correlations $\Delta \rho / \sqrt{\rho_{\mathrm{ref}}}$ on $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ for Au-Au collisions at $\sqrt{s_{N N}}=200$ and $62 \mathrm{GeV}$ (top and bottom rows, respectively). Centrality increases left to right from most peripheral to most central. Corrected total cross-section fractions are (left to right) $84 \%-93 \%, 55 \%-64 \%, 18 \%-28 \%,$ and $0 \%-5 \%$ for the $200-\mathrm{GeV}$ data and $84 \%-95 \%, 56 \%-65 \%$ $18 \%-28 \%,$ and $0 \%-5 \%$ for the $62 \mathrm{GeV}$ data (see Tables III and IV).
FIG. 1. (Color online) Perspective views of $2 \mathrm{D}$ charge-independent angular correlations $\Delta \rho / \sqrt{\rho_{\mathrm{ref}}}$ on $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ for Au-Au collisions at $\sqrt{s_{N N}}=200$ and $62 \mathrm{GeV}$ (top and bottom rows, respectively). Centrality increases left to right from most peripheral to most central. Corrected total cross-section fractions are (left to right) $84 \%-93 \%, 55 \%-64 \%, 18 \%-28 \%,$ and $0 \%-5 \%$ for the $200-\mathrm{GeV}$ data and $84 \%-95 \%, 56 \%-65 \%$ $18 \%-28 \%,$ and $0 \%-5 \%$ for the $62 \mathrm{GeV}$ data (see Tables III and IV).
FIG. 1. (Color online) Perspective views of $2 \mathrm{D}$ charge-independent angular correlations $\Delta \rho / \sqrt{\rho_{\mathrm{ref}}}$ on $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ for Au-Au collisions at $\sqrt{s_{N N}}=200$ and $62 \mathrm{GeV}$ (top and bottom rows, respectively). Centrality increases left to right from most peripheral to most central. Corrected total cross-section fractions are (left to right) $84 \%-93 \%, 55 \%-64 \%, 18 \%-28 \%,$ and $0 \%-5 \%$ for the $200-\mathrm{GeV}$ data and $84 \%-95 \%, 56 \%-65 \%$ $18 \%-28 \%,$ and $0 \%-5 \%$ for the $62 \mathrm{GeV}$ data (see Tables III and IV).
FIG. 1. (Color online) Perspective views of $2 \mathrm{D}$ charge-independent angular correlations $\Delta \rho / \sqrt{\rho_{\mathrm{ref}}}$ on $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ for Au-Au collisions at $\sqrt{s_{N N}}=200$ and $62 \mathrm{GeV}$ (top and bottom rows, respectively). Centrality increases left to right from most peripheral to most central. Corrected total cross-section fractions are (left to right) $84 \%-93 \%, 55 \%-64 \%, 18 \%-28 \%,$ and $0 \%-5 \%$ for the $200-\mathrm{GeV}$ data and $84 \%-95 \%, 56 \%-65 \%$ $18 \%-28 \%,$ and $0 \%-5 \%$ for the $62 \mathrm{GeV}$ data (see Tables III and IV).
FIG. 1. (Color online) Perspective views of $2 \mathrm{D}$ charge-independent angular correlations $\Delta \rho / \sqrt{\rho_{\mathrm{ref}}}$ on $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ for Au-Au collisions at $\sqrt{s_{N N}}=200$ and $62 \mathrm{GeV}$ (top and bottom rows, respectively). Centrality increases left to right from most peripheral to most central. Corrected total cross-section fractions are (left to right) $84 \%-93 \%, 55 \%-64 \%, 18 \%-28 \%,$ and $0 \%-5 \%$ for the $200-\mathrm{GeV}$ data and $84 \%-95 \%, 56 \%-65 \%$ $18 \%-28 \%,$ and $0 \%-5 \%$ for the $62 \mathrm{GeV}$ data (see Tables III and IV).
FIG. 1. (Color online) Perspective views of $2 \mathrm{D}$ charge-independent angular correlations $\Delta \rho / \sqrt{\rho_{\mathrm{ref}}}$ on $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ for Au-Au collisions at $\sqrt{s_{N N}}=200$ and $62 \mathrm{GeV}$ (top and bottom rows, respectively). Centrality increases left to right from most peripheral to most central. Corrected total cross-section fractions are (left to right) $84 \%-93 \%, 55 \%-64 \%, 18 \%-28 \%,$ and $0 \%-5 \%$ for the $200-\mathrm{GeV}$ data and $84 \%-95 \%, 56 \%-65 \%$ $18 \%-28 \%,$ and $0 \%-5 \%$ for the $62 \mathrm{GeV}$ data (see Tables III and IV).
FIG. 1. (Color online) Perspective views of $2 \mathrm{D}$ charge-independent angular correlations $\Delta \rho / \sqrt{\rho_{\mathrm{ref}}}$ on $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ for Au-Au collisions at $\sqrt{s_{N N}}=200$ and $62 \mathrm{GeV}$ (top and bottom rows, respectively). Centrality increases left to right from most peripheral to most central. Corrected total cross-section fractions are (left to right) $84 \%-93 \%, 55 \%-64 \%, 18 \%-28 \%,$ and $0 \%-5 \%$ for the $200-\mathrm{GeV}$ data and $84 \%-95 \%, 56 \%-65 \%$ $18 \%-28 \%,$ and $0 \%-5 \%$ for the $62 \mathrm{GeV}$ data (see Tables III and IV).
FIG. 2. (Color online) Fit decomposition of the $46 \%-56 \%$ centrality data for 62 -GeV Au-Au collisions. The top panels show from left to right the corrected data, model fit, fit residuals (data - model), and same-side 2D Gaussian. The bottom panels similarly show the away-side azimuth dipole, the nonjet azimuth quadrupole, the 1D $\eta_{\Delta}$ Gaussian, and the 2D exponential. This centrality is just below the sharp transition at $v_{\text {trans }}=3$. Fit residuals (c) are scaled up eightfold relative to the data.
FIG. 3. Fit parameters for $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ correlation data from Au-Au collisions at $\sqrt{s_{N N}}=62$ (open symbols) and 200 GeV (solid symbols) versus centrality measure $\nu$ computed at fixed energy $(200 \mathrm{GeV})$. The SS $2 \mathrm{D}$ Gaussian amplitudes, $\eta_{\Delta}$ widths, and $\phi_{\Delta}$ widths are shown in the left, center, and right panels, respectively of the top row. The bottom row shows from left to right the amplitudes for the dipole, quadrupole, and SS peak width aspect ratio $\sigma_{\eta_{\Delta}} / \sigma_{\phi_{\Delta}} .$ Fitting errors are indicated by error bars where larger than the symbols. Solid lines connect the points for clarity. The dotted and dashed curves indicate Glauber linear superposition estimates for 62 - and 200 -GeV peak amplitudes respectively, as discussed in the text. The quadrupole data are consistent with Ref. [60]. The hatched regions indicate the full range of systematic uncertainties listed in Appendix F. The vertical dark bands indicate estimated $v$ equivalents for $N-N$ collisions and $b=0$ Au-Au collisions.
FIG. 3. Fit parameters for $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ correlation data from Au-Au collisions at $\sqrt{s_{N N}}=62$ (open symbols) and 200 GeV (solid symbols) versus centrality measure $\nu$ computed at fixed energy $(200 \mathrm{GeV})$. The SS $2 \mathrm{D}$ Gaussian amplitudes, $\eta_{\Delta}$ widths, and $\phi_{\Delta}$ widths are shown in the left, center, and right panels, respectively of the top row. The bottom row shows from left to right the amplitudes for the dipole, quadrupole, and SS peak width aspect ratio $\sigma_{\eta_{\Delta}} / \sigma_{\phi_{\Delta}} .$ Fitting errors are indicated by error bars where larger than the symbols. Solid lines connect the points for clarity. The dotted and dashed curves indicate Glauber linear superposition estimates for 62 - and 200 -GeV peak amplitudes respectively, as discussed in the text. The quadrupole data are consistent with Ref. [60]. The hatched regions indicate the full range of systematic uncertainties listed in Appendix F. The vertical dark bands indicate estimated $v$ equivalents for $N-N$ collisions and $b=0$ Au-Au collisions.
FIG. 3. Fit parameters for $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ correlation data from Au-Au collisions at $\sqrt{s_{N N}}=62$ (open symbols) and 200 GeV (solid symbols) versus centrality measure $\nu$ computed at fixed energy $(200 \mathrm{GeV})$. The SS $2 \mathrm{D}$ Gaussian amplitudes, $\eta_{\Delta}$ widths, and $\phi_{\Delta}$ widths are shown in the left, center, and right panels, respectively of the top row. The bottom row shows from left to right the amplitudes for the dipole, quadrupole, and SS peak width aspect ratio $\sigma_{\eta_{\Delta}} / \sigma_{\phi_{\Delta}} .$ Fitting errors are indicated by error bars where larger than the symbols. Solid lines connect the points for clarity. The dotted and dashed curves indicate Glauber linear superposition estimates for 62 - and 200 -GeV peak amplitudes respectively, as discussed in the text. The quadrupole data are consistent with Ref. [60]. The hatched regions indicate the full range of systematic uncertainties listed in Appendix F. The vertical dark bands indicate estimated $v$ equivalents for $N-N$ collisions and $b=0$ Au-Au collisions.
FIG. 3. Fit parameters for $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ correlation data from Au-Au collisions at $\sqrt{s_{N N}}=62$ (open symbols) and 200 GeV (solid symbols) versus centrality measure $\nu$ computed at fixed energy $(200 \mathrm{GeV})$. The SS $2 \mathrm{D}$ Gaussian amplitudes, $\eta_{\Delta}$ widths, and $\phi_{\Delta}$ widths are shown in the left, center, and right panels, respectively of the top row. The bottom row shows from left to right the amplitudes for the dipole, quadrupole, and SS peak width aspect ratio $\sigma_{\eta_{\Delta}} / \sigma_{\phi_{\Delta}} .$ Fitting errors are indicated by error bars where larger than the symbols. Solid lines connect the points for clarity. The dotted and dashed curves indicate Glauber linear superposition estimates for 62 - and 200 -GeV peak amplitudes respectively, as discussed in the text. The quadrupole data are consistent with Ref. [60]. The hatched regions indicate the full range of systematic uncertainties listed in Appendix F. The vertical dark bands indicate estimated $v$ equivalents for $N-N$ collisions and $b=0$ Au-Au collisions.
FIG. 3. Fit parameters for $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ correlation data from Au-Au collisions at $\sqrt{s_{N N}}=62$ (open symbols) and 200 GeV (solid symbols) versus centrality measure $\nu$ computed at fixed energy $(200 \mathrm{GeV})$. The SS $2 \mathrm{D}$ Gaussian amplitudes, $\eta_{\Delta}$ widths, and $\phi_{\Delta}$ widths are shown in the left, center, and right panels, respectively of the top row. The bottom row shows from left to right the amplitudes for the dipole, quadrupole, and SS peak width aspect ratio $\sigma_{\eta_{\Delta}} / \sigma_{\phi_{\Delta}} .$ Fitting errors are indicated by error bars where larger than the symbols. Solid lines connect the points for clarity. The dotted and dashed curves indicate Glauber linear superposition estimates for 62 - and 200 -GeV peak amplitudes respectively, as discussed in the text. The quadrupole data are consistent with Ref. [60]. The hatched regions indicate the full range of systematic uncertainties listed in Appendix F. The vertical dark bands indicate estimated $v$ equivalents for $N-N$ collisions and $b=0$ Au-Au collisions.
FIG. 3. Fit parameters for $\left(\eta_{\Delta}, \phi_{\Delta}\right)$ correlation data from Au-Au collisions at $\sqrt{s_{N N}}=62$ (open symbols) and 200 GeV (solid symbols) versus centrality measure $\nu$ computed at fixed energy $(200 \mathrm{GeV})$. The SS $2 \mathrm{D}$ Gaussian amplitudes, $\eta_{\Delta}$ widths, and $\phi_{\Delta}$ widths are shown in the left, center, and right panels, respectively of the top row. The bottom row shows from left to right the amplitudes for the dipole, quadrupole, and SS peak width aspect ratio $\sigma_{\eta_{\Delta}} / \sigma_{\phi_{\Delta}} .$ Fitting errors are indicated by error bars where larger than the symbols. Solid lines connect the points for clarity. The dotted and dashed curves indicate Glauber linear superposition estimates for 62 - and 200 -GeV peak amplitudes respectively, as discussed in the text. The quadrupole data are consistent with Ref. [60]. The hatched regions indicate the full range of systematic uncertainties listed in Appendix F. The vertical dark bands indicate estimated $v$ equivalents for $N-N$ collisions and $b=0$ Au-Au collisions.
FIG. 4. (Color online) (a) 2D data histogram from $0 \%-5 \%$ central 200 GeV Au-Au collisions $[(0,0)$ bin suppressed]. (b) Additional model component fitted to the $2 \mathrm{D}$ histogram and consisting of an AS azimuth dipole modulated by function $F\left(\eta_{\Delta}\right)$ described in the text. (c) Fit residuals including the new model component. (d) Data histogram in the first panel minus the additional model component and fitted offset. Remaining structure is described accurately by an AS dipole and SS 2D Gaussian.
FIG. 9. (a) Amplitude of SS 2D peak (jet-correlated pairs per final-state hadron) for data (solid points), GLS extrapolation from $p$ - $p$ data (dashed curve) and from the HIJING Monte Carlo (open points, dotted curve). (b) Single-particle production extrapolated from $p-p$ data (dashed curve, GLS), and from more-central Au-Au data (solid line) and HIJING (dash-dotted line, open points). (c) Single-particle hard-component production per $N-N$ binary collision from $p-p$ data, from more-central Au-Au data and from HIJING (open points). (d) Jet-correlated pair production (SS 2D peak) per $N-N$ binary collision extrapolated from $p-p$ data (GLS), and from Au-Au data (solid points) and HIJING (open points).
FIG. 9. (a) Amplitude of SS 2D peak (jet-correlated pairs per final-state hadron) for data (solid points), GLS extrapolation from $p$ - $p$ data (dashed curve) and from the HIJING Monte Carlo (open points, dotted curve). (b) Single-particle production extrapolated from $p-p$ data (dashed curve, GLS), and from more-central Au-Au data (solid line) and HIJING (dash-dotted line, open points). (c) Single-particle hard-component production per $N-N$ binary collision from $p-p$ data, from more-central Au-Au data and from HIJING (open points). (d) Jet-correlated pair production (SS 2D peak) per $N-N$ binary collision extrapolated from $p-p$ data (GLS), and from Au-Au data (solid points) and HIJING (open points).
FIG. 9. (a) Amplitude of SS 2D peak (jet-correlated pairs per final-state hadron) for data (solid points), GLS extrapolation from $p$ - $p$ data (dashed curve) and from the HIJING Monte Carlo (open points, dotted curve). (b) Single-particle production extrapolated from $p-p$ data (dashed curve, GLS), and from more-central Au-Au data (solid line) and HIJING (dash-dotted line, open points). (c) Single-particle hard-component production per $N-N$ binary collision from $p-p$ data, from more-central Au-Au data and from HIJING (open points). (d) Jet-correlated pair production (SS 2D peak) per $N-N$ binary collision extrapolated from $p-p$ data (GLS), and from Au-Au data (solid points) and HIJING (open points).
FIG. 9. (a) Amplitude of SS 2D peak (jet-correlated pairs per final-state hadron) for data (solid points), GLS extrapolation from $p$ - $p$ data (dashed curve) and from the HIJING Monte Carlo (open points, dotted curve). (b) Single-particle production extrapolated from $p-p$ data (dashed curve, GLS), and from more-central Au-Au data (solid line) and HIJING (dash-dotted line, open points). (c) Single-particle hard-component production per $N-N$ binary collision from $p-p$ data, from more-central Au-Au data and from HIJING (open points). (d) Jet-correlated pair production (SS 2D peak) per $N-N$ binary collision extrapolated from $p-p$ data (GLS), and from Au-Au data (solid points) and HIJING (open points).
FIG. 11. (Color online) (Left) Uncorrected angular correlations from 62-GeV $37 \%-46 \%$ central Au-Au collisions showing pileup distortions, especially evident as the W-shaped nonuniformity of the AS ridge on $\eta_{\Delta}$. (Right) The same data with pileup correction applied.
We present STAR measurements of azimuthal anisotropy by means of the two- and four-particle cumulants $v_2$ ($v_2\{2\}$ and $v_2\{4\}$) for Au+Au and Cu+Cu collisions at center of mass energies $\sqrt{s_{_{\mathrm{NN}}}} = 62.4$ and 200 GeV. The difference between $v_2\{2\}^2$ and $v_2\{4\}^2$ is related to $v_{2}$ fluctuations ($\sigma_{v_2}$) and nonflow $(\delta_{2})$. We present an upper limit to $\sigma_{v_2}/v_{2}$. Following the assumption that eccentricity fluctuations $\sigma_{\epsilon}$ dominate $v_2$ fluctuations $\frac{\sigma_{v_2}}{v_2} \approx \frac{\sigma_{\epsilon}}{\epsilon}$ we deduce the nonflow implied for several models of eccentricity fluctuations that would be required for consistency with $v_2\{2\}$ and $v_2\{4\}$. We also present results on the ratio of $v_2$ to eccentricity.
The two-particle cumulant $v_2\{2\}^2$ for Au+Au collisions at 200 and 62.4 GeV. Results are shown with like-sign combinations (LS) and charge-independent results (CI) for $0.15 < p_T < 2.0$ GeV/$c$.
The two-particle cumulant $v_2\{2\}^2$ for Au+Au collisions at 200 and 62.4 GeV. Results are shown with like-sign combinations (LS) and charge-independent results (CI) for $0.15 < p_T < 2.0$ GeV/$c$.
The same as the left but for Cu+Cu collisions. The systematic errors are shown as thin lines with wide caps at the ends and statistical errors are shown as thick lines with small caps at the end. Statistical and systematic errors are very small.
The same as the left but for Cu+Cu collisions. The systematic errors are shown as thin lines with wide caps at the ends and statistical errors are shown as thick lines with small caps at the end. Statistical and systematic errors are very small.
The LS and CI four-particle cumulant $v_2\{4\}^4$ for Au+Au collisions at 200 and 62.4 GeV for $0.15 < pT < 2.0$ GeV/$c$. The systematic errors are shown as narrow lines with wide caps at the end and statistical errors are shown as thick lines with narrow caps at the end. Statistical errors are not visible for most of the points.
The LS and CI four-particle cumulant $v_2\{4\}^4$ for Au+Au collisions at 200 and 62.4 GeV for $0.15 < pT < 2.0$ GeV/$c$. The systematic errors are shown as narrow lines with wide caps at the end and statistical errors are shown as thick lines with narrow caps at the end. Statistical errors are not visible for most of the points.
The LS and CI four-particle cumulant $v_2\{4\}^4$ for Cu+Cu collisions at 200 and 62.4 GeV for $0.15 < p_T < 2.0$ GeV/c. The most central points (two points for Cu+Cu 62.4 GeV) gives $v_2\{4\}^4 < 0$ for all the data sets. The negative values are probably due to large fluctuations in agreement with Eq. (1). These may include contributions from impact parameter spread and finite multiplicity bin width.
The LS and CI four-particle cumulant $v_2\{4\}^4$ for Cu+Cu collisions at 200 and 62.4 GeV for $0.15 < p_T < 2.0$ GeV/c. The most central points (two points for Cu+Cu 62.4 GeV) gives $v_2\{4\}^4 < 0$ for all the data sets. The negative values are probably due to large fluctuations in agreement with Eq. (1). These may include contributions from impact parameter spread and finite multiplicity bin width.
The difference of charge-independent (CI) $v_2\{4\}$ and like-sign (LS) $v_2\{4\}$ for Au+Au collisions at 200 and 62.4 GeV vs. the log of $\langle dN_{ch}/d\eta\rangle$.
The difference of charge-independent (CI) $v_2\{4\}$ and like-sign (LS) $v_2\{4\}$ for Au+Au collisions at 200 and 62.4 GeV vs. the log of $\langle dN_{ch}/d\eta\rangle$.
The upper limit on $\sigma_{v_2}/\langle v_2 \rangle$ for 200 GeV (left) and 62.4 GeV (right) Au+Au collisions from Eq. (9) compared to $\sigma_\varepsilon/\varepsilon$ from Eq. (10) for three different models. The upper limit is found using the LS results for $v_2\{2\}$. Data are from the range $0.15 < p_T < 2.0$ GeV/$c$. The shaded bands reflect the uncertainties on the models which are dominated by uncertainty on the distribution of nucleons inside the nucleus. The uncertainty is only shown for the MCG-N and fKLN-CGC models. The uncertainty on the MCG-Q model is the same as for the MCG-N model but is not shown for the visual clarity.
The upper limit on $\sigma_{v_2}/\langle v_2 \rangle$ for 200 GeV (left) and 62.4 GeV (right) Au+Au collisions from Eq. (9) compared to $\sigma_\varepsilon/\varepsilon$ from Eq. (10) for three different models. The upper limit is found using the LS results for $v_2\{2\}$. Data are from the range $0.15 < p_T < 2.0$ GeV/$c$. The shaded bands reflect the uncertainties on the models which are dominated by uncertainty on the distribution of nucleons inside the nucleus. The uncertainty is only shown for the MCG-N and fKLN-CGC models. The uncertainty on the MCG-Q model is the same as for the MCG-N model but is not shown for the visual clarity.
The upper limit on $\sigma_{v_2}/\langle v_2 \rangle$ for 200 GeV (left) and 62.4 GeV (right) Au+Au collisions from Eq. (9) compared to $\sigma_\varepsilon/\varepsilon$ from Eq. (10) for three different models. The upper limit is found using the LS results for $v_2\{2\}$. Data are from the range $0.15 < p_T < 2.0$ GeV/$c$. The shaded bands reflect the uncertainties on the models which are dominated by uncertainty on the distribution of nucleons inside the nucleus. The uncertainty is only shown for the MCG-N and fKLN-CGC models. The uncertainty on the MCG-Q model is the same as for the MCG-N model but is not shown for the visual clarity.
The upper limit on $\sigma_{v_2}/\langle v_2 \rangle$ for 200 GeV (left) and 62.4 GeV (right) Au+Au collisions from Eq. (9) compared to $\sigma_\varepsilon/\varepsilon$ from Eq. (10) for three different models. The upper limit is found using the LS results for $v_2\{2\}$. Data are from the range $0.15 < p_T < 2.0$ GeV/$c$. The shaded bands reflect the uncertainties on the models which are dominated by uncertainty on the distribution of nucleons inside the nucleus. The uncertainty is only shown for the MCG-N and fKLN-CGC models. The uncertainty on the MCG-Q model is the same as for the MCG-N model but is not shown for the visual clarity.
The STAR data compared to PHOBOS data [34] on $\sigma_{v_2}/\langle v_2 \rangle$ with $\delta_2$ for $\Delta\eta > 2$ taken to be zero (see Fig. 6 from Ref. [34]). The shaded band shows the errors quoted from Ref. [34].
The STAR data compared to PHOBOS data [34] on $\sigma_{v_2}/\langle v_2 \rangle$ with $\delta_2$ for $\Delta\eta > 2$ taken to be zero (see Fig. 6 from Ref. [34]). The shaded band shows the errors quoted from Ref. [34].
The upper limit on $\sigma_{v_2}/\langle v_2 \rangle$ for 200 GeV (left) and 62.4 GeV (right) Cu+Cu collisions from Eq. (9) compared to $\sigma_\varepsilon/\varepsilon$ from Eq. (10) for three different models.
The upper limit on $\sigma_{v_2}/\langle v_2 \rangle$ for 200 GeV (left) and 62.4 GeV (right) Cu+Cu collisions from Eq. (9) compared to $\sigma_\varepsilon/\varepsilon$ from Eq. (10) for three different models.
The upper limit on $\sigma_{v_2}/\langle v_2 \rangle$ for 200 GeV (left) and 62.4 GeV (right) Cu+Cu collisions from Eq. (9) compared to $\sigma_\varepsilon/\varepsilon$ from Eq. (10) for three different models.
The upper limit on $\sigma_{v_2}/\langle v_2 \rangle$ for 200 GeV (left) and 62.4 GeV (right) Cu+Cu collisions from Eq. (9) compared to $\sigma_\varepsilon/\varepsilon$ from Eq. (10) for three different models.
We report the first measurements of the kurtosis (\kappa), skewness (S) and variance (\sigma^2) of net-proton multiplicity (N_p - N_pbar) distributions at midrapidity for Au+Au collisions at \sqrt(s_NN) = 19.6, 62.4, and 200 GeV corresponding to baryon chemical potentials (\mu_B) between 200 - 20 MeV. Our measurements of the products \kappa \sigma^2 and S \sigma, which can be related to theoretical calculations sensitive to baryon number susceptibilities and long range correlations, are constant as functions of collision centrality. We compare these products with results from lattice QCD and various models without a critical point and study the \sqrt(s_NN) dependence of \kappa \sigma^2. From the measurements at the three beam energies, we find no evidence for a critical point in the QCD phase diagram for \mu_B below 200 MeV.
STAR measurements of dihadron azimuthal correlations ($\Delta\phi$) are reported 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 elliptic ($v_2$), triangular ($v_3$), and quadratic ($v_4$) flow harmonic backgrounds are subtracted using the Zero Yield At Minimum (ZYAM) method. The results are compared to minimum-bias d+Au collisions. It is found that a finite near-side ($|\Delta\phi|<\pi/2$) long-range pseudorapidity correlation (ridge) is present in the in-plane direction ($\phi_{s}\sim 0$). The away-side ($|\Delta\phi|>\pi/2$) correlation shows a modification from d+Au data, varying with $\phi_{s}$. The modification may be a consequence of pathlength-dependent jet-quenching and may lead to a better understanding of high-density QCD.
raw correlation, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 0.
raw correlation, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 1.
raw correlation, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 2.
raw correlation, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 3.
raw correlation, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 4.
raw correlation, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 5.
flow background with default flow, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 0.
flow background with default flow, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 1.
flow background with default flow, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 2.
flow background with default flow, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 3.
flow background with default flow, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 4.
flow background with default flow, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 5.
flow background with upper flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 0.
flow background with upper flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 1.
flow background with upper flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 2.
flow background with upper flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 3.
flow background with upper flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 4.
flow background with upper flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 5.
flow background with lower flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 0.
flow background with lower flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 1.
flow background with lower flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 2.
flow background with lower flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 3.
flow background with lower flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 4.
flow background with lower flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 5.
background-subtracted correlation, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 0.
background-subtracted correlation, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 1.
background-subtracted correlation, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 2.
background-subtracted correlation, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 3.
background-subtracted correlation, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 4.
background-subtracted correlation, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 5.
background-subtracted correlation with upper flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 0.
background-subtracted correlation with upper flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 1.
background-subtracted correlation with upper flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 2.
background-subtracted correlation with upper flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 3.
background-subtracted correlation with upper flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 4.
background-subtracted correlation with upper flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 5.
background-subtracted correlation with lower flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 0.
background-subtracted correlation with lower flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 1.
background-subtracted correlation with lower flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 2.
background-subtracted correlation with lower flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 3.
background-subtracted correlation with lower flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 4.
background-subtracted correlation with lower flow systematic uncertainty, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 5.
background normalization systematic uncertainty band, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 0.
background normalization systematic uncertainty band, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 1.
background normalization systematic uncertainty band, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 2.
background normalization systematic uncertainty band, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 3.
background normalization systematic uncertainty band, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 4.
background normalization systematic uncertainty band, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1, slice 5.
d+Au background-subtracted correlation, Au+Au 200 GeV, 20-60%, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, |#eta|<1.
Parameters of Gaussian fit to the background subtracted dihadron correlations as a function of phi_s.
Parameters of Gaussian fit to the background subtracted dihadron correlations as a function of phi_s.
Parameters of Gaussian fit to the background subtracted dihadron correlations as a function of phi_s.
Parameters of Gaussian fit to the background subtracted dihadron correlations as a function of phi_s.
Parameters of Gaussian fit to the background subtracted dihadron correlations as a function of phi_s.
Parameters of Gaussian fit to the background subtracted dihadron correlations as a function of phi_s.
Parameters of Gaussian fit to the background subtracted dihadron correlations as a function of phi_s.
Parameters of Gaussian fit to the background subtracted dihadron correlations as a function of phi_s.
Parameters of Gaussian fit to the background subtracted dihadron correlations as a function of phi_s.
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