Showing 10 of 28 results
None
The absolute value of the π 0 photoproduction cross section on the proton recently measured near threshold enables to reanalyze previous data collected on 2 H, 3 He, and 4 He relatively to the proton. Absolute cross sections are presented for these nuclei in the energy region extending up to 10 MeV above threshold. The threshold s-wave amplitudes for 2 H and 3 He thus obtained are discussed in relation with the neutron threshold amplitude E ( nπ 0 ) 0+ value.
We report the beam energy (\sqrt s_{NN} = 7.7 - 200 GeV) and collision centrality dependence of the mean (M), standard deviation (\sigma), skewness (S), and kurtosis (\kappa) of the net-proton multiplicity distributions in Au+Au collisions. The measurements are carried out by the STAR experiment at midrapidity (|y| < 0.5) and within the transverse momentum range 0.4 < pT < 0.8 GeV/c in the first phase of the Beam Energy Scan program at the Relativistic Heavy Ion Collider. These measurements are important for understanding the Quantum Chromodynamic (QCD) phase diagram. The products of the moments, S\sigma and \kappa\sigma^{2}, are sensitive to the correlation length of the hot and dense medium created in the collisions and are related to the ratios of baryon number susceptibilities of corresponding orders. The products of moments are found to have values significantly below the Skellam expectation and close to expectations based on independent proton and anti-proton production. The measurements are compared to a transport model calculation to understand the effect of acceptance and baryon number conservation, and also to a hadron resonance gas model.
$\Delta N_p$ multiplicity distributions in Au+Au collisions at $\sqrt{S_{NN}}=7.7$ GeV for 0-5 percent, 30-40 percent and 70-80 percent collision centralities at midrapidity.
$\Delta N_p$ multiplicity distributions in Au+Au collisions at $\sqrt{S_{NN}}=11.5$ GeV for 0-5 percent, 30-40 percent and 70-80 percent collision centralities at midrapidity.
$\Delta N_p$ multiplicity distributions in Au+Au collisions at $\sqrt{S_{NN}}=19.6$ GeV for 0-5 percent, 30-40 percent and 70-80 percent collision centralities at midrapidity.
$\Delta N_p$ multiplicity distributions in Au+Au collisions at $\sqrt{S_{NN}}=27$ GeV for 0-5 percent, 30-40 percent and 70-80 percent collision centralities at midrapidity.
$\Delta N_p$ multiplicity distributions in Au+Au collisions at $\sqrt{S_{NN}}=39$ GeV for 0-5 percent, 30-40 percent and 70-80 percent collision centralities at midrapidity.
$\Delta N_p$ multiplicity distributions in Au+Au collisions at $\sqrt{S_{NN}}=62.4$ GeV for 0-5 percent, 30-40 percent and 70-80 percent collision centralities at midrapidity.
$\Delta N_p$ multiplicity distributions in Au+Au collisions at $\sqrt{S_{NN}}=200$ GeV for 0-5 percent, 30-40 percent and 70-80 percent collision centralities at midrapidity.
A first measurement is presented of exclusive photoproduction of $\rho^0$ mesons associated with leading neutrons at HERA. The data were taken with the H1 detector in the years $2006$ and $2007$ at a centre-of-mass energy of $\sqrt{s}=319$ GeV and correspond to an integrated luminosity of $1.16$ pb$^{-1}$. The $\rho^0$ mesons with transverse momenta $p_T<1$ GeV are reconstructed from their decays to charged pions, while leading neutrons carrying a large fraction of the incoming proton momentum, $x_L>0.35$, are detected in the Forward Neutron Calorimeter. The phase space of the measurement is defined by the photon virtuality $Q^2 < 2$ GeV$^2$, the total energy of the photon-proton system $20 < W_{\gamma p} < 100$ GeV and the polar angle of the leading neutron $\theta_n < 0.75$ mrad. The cross section of the reaction $\gamma p \to \rho^0 n \pi^+$ is measured as a function of several variables. The data are interpreted in terms of a double peripheral process, involving pion exchange at the proton vertex followed by elastic photoproduction of a $\rho^0$ meson on the virtual pion. In the framework of one-pion-exchange dominance the elastic cross section of photon-pion scattering, $\sigma^{\rm el}(\gamma\pi^+ \to \rho^0\pi^+)$, is extracted. The value of this cross section indicates significant absorptive corrections for the exclusive reaction $\gamma p\to\rho^0 n \pi^+$.
Energy dependence of the exclusive photoproduction of a $\rho^0$ meson associated with a leading neutron, $\gamma p \to \rho^0 n \pi^+$. The first uncertainty is statistical and the second is systematic. The global normalisation uncertainty of $4.4\%$ is not included. $\Phi_{\gamma}$ is the integral of the photon flux, Eq. (3) of paper, in a given $W_{\gamma p}$ bin.
A combination is presented of all inclusive deep inelastic cross sections previously published by the H1 and ZEUS collaborations at HERA for neutral and charged current $e^{\pm}p$ scattering for zero beam polarisation. The data were taken at proton beam energies of 920, 820, 575 and 460 GeV and an electron beam energy of 27.5 GeV. The data correspond to an integrated luminosity of about 1 fb$^{-1}$ and span six orders of magnitude in negative four-momentum-transfer squared, $Q^2$, and Bjorken $x$. The correlations of the systematic uncertainties were evaluated and taken into account for the combination. The combined cross sections were input to QCD analyses at leading order, next-to-leading order and at next-to-next-to-leading order, providing a new set of parton distribution functions, called HERAPDF2.0. In addition to the experimental uncertainties, model and parameterisation uncertainties were assessed for these parton distribution functions. Variants of HERAPDF2.0 with an alternative gluon parameterisation, HERAPDF2.0AG, and using fixed-flavour-number schemes, HERAPDF2.0FF, are presented. The analysis was extended by including HERA data on charm and jet production, resulting in the variant HERAPDF2.0Jets. The inclusion of jet-production cross sections made a simultaneous determination of these parton distributions and the strong coupling constant possible, resulting in $\alpha_s(M_Z)=0.1183 \pm 0.0009 {\rm(exp)} \pm 0.0005{\rm (model/parameterisation)} \pm 0.0012{\rm (hadronisation)} ^{+0.0037}_{-0.0030}{\rm (scale)}$. An extraction of $xF_3^{\gamma Z}$ and results on electroweak unification and scaling violations are also presented.
Collisions between prolate uranium nuclei are used to study how particle production and azimuthal anisotropies depend on initial geometry in heavy-ion collisions. We report the two- and four-particle cumulants, $v_2\{2\}$ and $v_2\{4\}$, for charged hadrons from U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV and Au+Au collisions at $\sqrt{s_{\rm NN}}$ = 200 GeV. Nearly fully overlapping collisions are selected based on the amount of energy deposited by spectators in the STAR Zero Degree Calorimeters (ZDCs). Within this sample, the observed dependence of $v_2\{2\}$ on multiplicity demonstrates that ZDC information combined with multiplicity can preferentially select different overlap configurations in U+U collisions. An initial-state model with gluon saturation describes the slope of $v_2\{2\}$ as a function of multiplicity in central collisions better than one based on Glauber with a two-component multiplicity model.
Dihadron angular correlations in $d$+Au collisions at $\sqrt{s_{\rm NN}}=200$ GeV are reported as a function of the measured zero-degree calorimeter neutral energy and the forward charged hadron multiplicity in the Au-beam direction. A finite correlated yield is observed at large relative pseudorapidity ($\Delta\eta$) on the near side (i.e. relative azimuth $\Delta\phi\sim0$). This correlated yield as a function of $\Delta\eta$ appears to scale with the dominant, primarily jet-related, away-side ($\Delta\phi\sim\pi$) yield. The Fourier coefficients of the $\Delta\phi$ correlation, $V_{n}=\langle\cos n\Delta\phi\rangle$, have a strong $\Delta\eta$ dependence. In addition, it is found that $V_{1}$ is approximately inversely proportional to the mid-rapidity event multiplicity, while $V_{2}$ is independent of it with similar magnitude in the forward ($d$-going) and backward (Au-going) directions.
The $\Delta\eta$ dependence of the ratio of the near- to away-side correlated yields in d+Au collisions. Positive(negative) $\eta$ corresponds to d(Au)-going direction. Only high ZDC-Au activity data are shown.
Fourier coefficient V1 versus the measured mid-rapidity charged particle $dN_{ch}/d\eta$. Event activity selection is by FTPC-Au. Trigger particles are from TPC, and associated particles from TPC. Systematic uncertainties are estimated to be 10% on V1. Errors shown are the quadratic sum of statistical and systematic errors.
Fourier coefficient V1 versus the measured mid-rapidity charged particle $dN_{ch}/d\eta$. Event activity selection is by ZDC. Trigger particles are from TPC, and associated particles from FTPC-Au. Systematic uncertainties are estimated to be 10% on V1. Errors shown are the quadratic sum of statistical and systematic errors.
Fourier coefficient V1 versus the measured mid-rapidity charged particle $dN_{ch}/d\eta$. Event activity selection is by ZDC. Trigger particles are from TPC, and associated particles from FTPC-d. Systematic uncertainties are estimated to be 10% on V1. Errors shown are the quadratic sum of statistical and systematic errors.
Fourier coefficient V1 versus the measured mid-rapidity charged particle $dN_{ch}/d\eta$. Event activity selection is by ZDC-Au. Trigger particles are from TPC, and associated particles from TPC. Systematic uncertainties are estimated to be 10% on V1. Errors shown are the quadratic sum of statistical and systematic errors.
A study is reported of the same- and opposite-sign charge-dependent azimuthal correlations with respect to the event plane in Au+Au collisions at 200 GeV. The charge multiplicity asymmetries between the up/down and left/right hemispheres relative to the event plane are utilized. The contributions from statistical fluctuations and detector effects were subtracted from the (co-)variance of the observed charge multiplicity asymmetries. In the mid- to most-central collisions, the same- (opposite-) sign pairs are preferentially emitted in back-to-back (aligned on the same-side) directions. The charge separation across the event plane, measured by the difference, $\Delta$, between the like- and unlike-sign up/down $-$ left/right correlations, is largest near the event plane. The difference is found to be proportional to the event-by-event final-state particle ellipticity (via the observed second-order harmonic $v^{\rm obs}_{2}$), where $\Delta=(1.3\pm1.4({\rm stat})^{+4.0}_{-1.0}({\rm syst}))\times10^{-5}+(3.2\pm0.2({\rm stat})^{+0.4}_{-0.3}({\rm syst}))\times10^{-3}v^{\rm obs}_{2}$ for 20-40% Au+Au collisions. The implications for the proposed chiral magnetic effect are discussed.
Centrality dependences of the charge asymmetry dynamical correlations, $\delta\langle A^{2}\rangle$, and the positive and negative charge asymmetry correlations, $\delta\langle A_{+}A_{-}\rangle$. The asymmetries are calculated between hemispheres separated by the event plane (UD) and between those separated by the plane perpendicular to the event plane (LR). The asymmetry correlations are multiplied by the number of participants $N_{part}$. The upper (lower) shaded band shows half of the systematic uncertainty in the $\delta\langle A_{+}A_{-}\rangle$ ($\delta\langle A^{2}\rangle$); the larger of the UD\ and LR\ systematic uncertainties is drawn. The stars and triangles depict the $d$+Au results.
The correlation differences $\Delta\langle A^{2}\rangle=\delta\langle A^{2}_{ UD}\rangle-\delta\langle A^{2}_{ LR}\rangle$ and $\Delta\langle A_{+}A_{-}\rangle=\delta\langle A_{+}A_{-}\rangle_{ UD}-\delta\langle A_{+}A_{-}\rangle_{ LR}$, scaled by the number of participants $N_{part}$, as a function of $N_{part}$. The error bars are statistical, and the systematic uncertainties are shown in the shaded bands (upper band for $\Delta\langle A_{+}A_{-}\rangle$ and lower band for $\Delta\langle A^{2}\rangle$). Also shown as the lines are the linear-extrapolated values of $\Delta\langle A^{2}\rangle$ and $\Delta\langle A_{+}A_{-}\rangle$ corresponding to a perfect event-plane resolution. The star and triangle depict the $d$+Au results.
The $p_{T}$ dependence of the charge asymmetry dynamical correlations, $\delta\langle A^{2}\rangle$, and the positive and negative charge asymmetry correlations, $\delta\langle A_{+}A_{-}\rangle$. The data are from 20-40% central Au+Au collisions. The asymmetries are calculated between hemispheres separated by the event plane (UD) and between those separated by the plane perpendicular to the event plane (LR).
The correlation differences $\Delta\langle A^{2}\rangle=\delta\langle A^{2}_{UD}\rangle-\delta\langle A^{2}_{ LR}\rangle$ and $\Delta\langle A_{+}A_{-}\rangle=\delta\langle A_{+}A_{-}\rangle_{ UD}-\delta\langle A_{+}A_{-}\rangle_{ LR}$ as a function of $p_{T}$. The data are from 20-40% central (upper) and 0-20% central (lower) Au+Au collisions.
The charge asymmetry correlations $\delta\langle A^{2}\rangle$ (left panels) and $\delta\langle A_{+}A_{-}\rangle$ (center panels), and correlation differences $\Delta\langle A^{2}\rangle=\delta\langle A^{2}_{ UD}\rangle-\delta\langle A^{2}_{ LR}\rangle$ and $\Delta\langle A_{+}A_{-}\rangle=\delta\langle A_{+}A_{-}\rangle_{ UD}-\delta\langle A_{+}A_{-}\rangle_{ LR}$ (right panels), as a function of the azimuthal elliptic anisotropy of high-$p_{T}$ ($p_{T}>2$~GeV/$c$) particles (upper panels) and low-$p_{T}$ ($p_{T}<2$~GeV/$c$) particles (lower panels). Data are from 20-40% Au+Au collisions. The particle $p_{T}$ range of $0.15<p_{T}<2$~GeV/$c$ is used for both EP construction and asymmetry calculation.
The charge asymmetry correlations $\delta\langle A^{2}\rangle$ (left panels) and $\delta\langle A_{+}A_{-}\rangle$ (center panels), and correlation differences $\Delta\langle A^{2}\rangle=\delta\langle A^{2}_{ UD}\rangle-\delta\langle A^{2}_{ LR}\rangle$ and $\Delta\langle A_{+}A_{-}\rangle=\delta\langle A_{+}A_{-}\rangle_{ UD}-\delta\langle A_{+}A_{-}\rangle_{ LR}$ (right panels), as a function of the azimuthal elliptic anisotropy of high-$p_{T}$ ($p_{T}>2$~GeV/$c$) particles (upper panels) and low-$p_{T}$ ($p_{T}<2$~GeV/$c$) particles (lower panels). Data are from 20-40% Au+Au collisions. The particle $p_{T}$ range of $0.15<p_{T}<2$~GeV/$c$ is used for both EP construction and asymmetry calculation.
The wedge size dependences of charge multiplicity asymmetry correlations (upper panel), and their differences between out-of-plane and in-plane, $\Delta\langle A^{2}\rangle$ and $\Delta\langle A_{+}A_{-}\rangle$ (lower panel) for 20-40% central Au+Au collisions.
The wedge size dependences of charge multiplicity asymmetry correlations (upper panel), and their differences between out-of-plane and in-plane, $\Delta\langle A^{2}\rangle$ and $\Delta\langle A_{+}A_{-}\rangle$ (lower panel) for 20-40% central Au+Au collisions.
Charge multiplicity asymmetry correlations as a function of the wedge location, $\phi_{ w}$, in 20-40% central Au+Au collisions. The wedge size is $30^{\circ}$. The curves are the characteristic $\cos(2\phi_{ w}$) to guide the eye.
The wedge size dependence of the difference between the same-sign and opposite-sign, $\Delta\langle A^{2}\rangle-\Delta\langle A_{+}A_{-}\rangle$.
The values of $\Delta\langle A^{2}\rangle-\Delta\langle A_{+}A_{-}\rangle$, scaled by $N_{part}$, as a function of the measured average elliptic anisotropy $<v^{obs}_{2}}>$ in Au+Au collisions. The centrality bin number is labeled by each data point, 0 for 70-80% up to 8 for 0-5%.
$\Delta=\Delta\langle A^{2}\rangle-\Delta\langle A_{+}A_{-}\rangle$ as a function of $v^{obs}_{2}$, the event-by-event elliptical anisotropy of particle distributions relative to the second-harmonic event plane reconstructed from TPC tracks (left panel) and the first harmonic event plane reconstructed from the ZDC-SMD neutron signals (middle panel), in 20-40% central Au+Au collisions. Right panel: Average $\Delta$ for events with $|v^{obs}_{2}|<0.04$ relative to the TPC event plane as a function of centrality.
$\Delta=\Delta\langle A^{2}\rangle-\Delta\langle A_{+}A_{-}\rangle$ as a function of $v^{obs}_{2}$, the event-by-event elliptical anisotropy of particle distributions relative to the second-harmonic event plane reconstructed from TPC tracks (left panel) and the first harmonic event plane reconstructed from the ZDC-SMD neutron signals (middle panel), in 20-40% central Au+Au collisions. Right panel: Average $\Delta$ for events with $|v^{obs}_{2}|<0.04$ relative to the TPC event plane as a function of centrality.
$\Delta=\Delta\langle A^{2}\rangle-\Delta\langle A_{+}A_{-}\rangle$ as a function of $v^{obs}_{2}$, the event-by-event elliptical anisotropy of particle distributions relative to the second-harmonic event plane reconstructed from TPC tracks (left panel) and the first harmonic event plane reconstructed from the ZDC-SMD neutron signals (middle panel), in 20-40% central Au+Au collisions. Right panel: Average $\Delta$ for events with $|v^{obs}_{2}|<0.04$ relative to the TPC event plane as a function of centrality.
Left panel: $\Delta\langle A^{2}\rangle$ and $\Delta\langle A_{+}A_{-}\rangle$ as a function of $v^{obs}_{2}$ with a random EP in 20-40% Au+Au collisions. The lines depict the results with reconstructed EP lower right panel for comparison. Middle panel: The differences in $\Delta\langle A^{2}\rangle$ and $\Delta\langle A_{+}A_{-}\rangle$ between the reconstructed EP and random EP results, respectively. Right panel: $\Delta=\Delta\langle A^{2}\rangle-\Delta\langle A_{+}A_{-}\rangle$ as a function of $v^{obs}_{2}$ with a random EP (open triangles).
Left panel: $\Delta\langle A^{2}\rangle$ and $\Delta\langle A_{+}A_{-}\rangle$ as a function of $v^{obs}_{2}$ with a random EP in 20-40% Au+Au collisions. The lines depict the results with reconstructed EP lower right panel for comparison. Middle panel: The differences in $\Delta\langle A^{2}\rangle$ and $\Delta\langle A_{+}A_{-}\rangle$ between the reconstructed EP and random EP results, respectively. Right panel: $\Delta=\Delta\langle A^{2}\rangle-\Delta\langle A_{+}A_{-}\rangle$ as a function of $v^{obs}_{2}$ with a random EP (open triangles).
Left panel: $\Delta\langle A^{2}\rangle$ and $\Delta\langle A_{+}A_{-}\rangle$ as a function of $v^{obs}_{2}$ with a random EP in 20-40% Au+Au collisions. The lines depict the results with reconstructed EP lower right panel for comparison. Middle panel: The differences in $\Delta\langle A^{2}\rangle$ and $\Delta\langle A_{+}A_{-}\rangle$ between the reconstructed EP and random EP results, respectively. Right panel: $\Delta=\Delta\langle A^{2}\rangle-\Delta\langle A_{+}A_{-}\rangle$ as a function of $v^{obs}_{2}$ with a random EP (open triangles).
The correlation differences, $\langle A^{2}_{ LR}\rangle-\langle A^{2}_{ UD}\rangle$ and $\langle A_{+}A_{-}\rangle_{ LR}-\langle A_{+}A_{-}\rangle_{ UD}$, scaled by the number of participants $(\pi/4)^2 N_{part}$. Also shown are $\langle \cos(\phi_{\alpha}+\phi_{\beta}-2\phi_{c})\rangle/v_{2,c} \approx \langle \cos(\phi_{\alpha}+\phi_{\beta}-2\psi_{ RP}) \rangle$ of same- and opposite-sign particle pairs ($\alpha$ and $\beta$) calculated from particles used for the charge asymmetry correlations with particle $c$ from those used for EP construction. The upper panel shows the default results where particles are divided according to $\eta$; the lower panel shows results with particles divided randomly into two halves and compared to published correlators.
The correlation differences, $\langle A^{2}_{ LR}\rangle-\langle A^{2}_{ UD}\rangle$ and $\langle A_{+}A_{-}\rangle_{ LR}-\langle A_{+}A_{-}\rangle_{ UD}$, scaled by the number of participants $(\pi/4)^2 N_{part}$. Also shown are $\langle \cos(\phi_{\alpha}+\phi_{\beta}-2\phi_{c})\rangle/v_{2,c} \approx \langle \cos(\phi_{\alpha}+\phi_{\beta}-2\psi_{ RP}) \rangle$ of same- and opposite-sign particle pairs ($\alpha$ and $\beta$) calculated from particles used for the charge asymmetry correlations with particle $c$ from those used for EP construction. The upper panel shows the default results where particles are divided according to $\eta$; the lower panel shows results with particles divided randomly into two halves and compared to published correlators.
Upper panel: Positively charged particle multiplicity distributions versus the azimuthal angle, $\phi$, in 30-40% central Au+Au collisions. The data are shown separately for $\eta>0$ and $\eta<0$. The magnetic polarities of the STAR magnet have been summed and the $p_{T}$ is integrated over the range $0.15<p_{T}<2$~GeV/$c$. The inverse of these distributions, properly normalized, were used to correct for the track efficiency versus $\phi$. Lower panel: Reconstructed event-plane azimuthal angle distributions in 30-40% central Au+Au collisions. Particles within $0.15 < p_{T} < 2$~GeV/$c$ from $\eta<0$ and $\eta>0$ were used separately to reconstruct the EP.
Upper panel: Positively charged particle multiplicity distributions versus the azimuthal angle, $\phi$, in 30-40% central Au+Au collisions. The data are shown separately for $\eta>0$ and $\eta<0$. The magnetic polarities of the STAR magnet have been summed and the $p_{T}$ is integrated over the range $0.15<p_{T}<2$~GeV/$c$. The inverse of these distributions, properly normalized, were used to correct for the track efficiency versus $\phi$. Lower panel: Reconstructed event-plane azimuthal angle distributions in 30-40% central Au+Au collisions. Particles within $0.15 < p_{T} < 2$~GeV/$c$ from $\eta<0$ and $\eta>0$ were used separately to reconstruct the EP.
The relative charge asymmetry correlations, $\langle A_{+}A_{-}\rangle_{ UD}/\langle A_{+}A_{-}\rangle_{ LR}$, as a function of the number of participants, $N_{part}$, for four combinations of $\eta$ ranges used for EP reconstruction and asymmetry calculation.
The asymmetry correlations, $\langle A^{2}_{+,{ UD}}\rangle$ (left panel), $\langle A^{2}_{-,{ UD}}\rangle$ (middle panel), and $\langle A_{+}A_{-}\rangle_{ UD}$ (right panel), multiplied by the number of participants $N_{part}$, before and after the corrections for the $\phi$-dependent acceptance $\times$ efficiency. The colored curves are the corresponding statistical fluctuations and detector effects. The results are separated for $\eta>0$ and $\eta<0$. Only $\eta>0$ is shown for $\langle A^{2}_{+,{ UD}}\rangle$ and $\eta<0$ for $\langle A^{2}_{-,{ UD}}\rangle$ for clarity.
The asymmetry correlations, $\langle A^{2}_{+,{ UD}}\rangle$ (left panel), $\langle A^{2}_{-,{ UD}}\rangle$ (middle panel), and $\langle A_{+}A_{-}\rangle_{ UD}$ (right panel), multiplied by the number of participants $N_{part}$, before and after the corrections for the $\phi$-dependent acceptance $\times$ efficiency. The colored curves are the corresponding statistical fluctuations and detector effects. The results are separated for $\eta>0$ and $\eta<0$. Only $\eta>0$ is shown for $\langle A^{2}_{+,{ UD}}\rangle$ and $\eta<0$ for $\langle A^{2}_{-,{ UD}}\rangle$ for clarity.
The asymmetry correlations, $\langle A^{2}_{+,{ UD}}\rangle$ (left panel), $\langle A^{2}_{-,{ UD}}\rangle$ (middle panel), and $\langle A_{+}A_{-}\rangle_{ UD}$ (right panel), multiplied by the number of participants $N_{part}$, before and after the corrections for the $\phi$-dependent acceptance $\times$ efficiency. The colored curves are the corresponding statistical fluctuations and detector effects. The results are separated for $\eta>0$ and $\eta<0$. Only $\eta>0$ is shown for $\langle A^{2}_{+,{ UD}}\rangle$ and $\eta<0$ for $\langle A^{2}_{-,{ UD}}\rangle$ for clarity.
Left panel: Statistical fluctuation and detector effects in the charge asymmetry variance (multiplied by the number of participants $N_{part}$) from the $\eta<0$ region. The dotted curve shows the $1/N$ approximation, the dashed curve shows the statistical fluctuations $\langle A^{2}_{-,{ LR,stat}}\rangle$ obtained by the (50-50) method (see the text). The solid curve connecting the solid points shows the net effect of the statistical fluctuations and detector non-uniformities, $\langle A^{2}_{-,{ LR,stat+det}}\rangle$, obtained by the adding-$\pi$ method, and the crosses shows the same but obtained from the ``scramble'' method. See the text for details. Middle panel: The statistical fluctuation effects relative to the $1/N$ approximation (thin curves) and the effects due to the imperfect detector (thick curves). The dashed curves are for the region $\eta>0$ and the solid curves are for $\eta<0$. Right panel: The ratios of the statistical fluctuation and detector effects $\langle A^{2}_{+,{ LR,stat+det}}\rangle/\langle A^{2}_{-,{ LR,stat+det}}\rangle$ and $\langle A^{2}_{+,{ UD,stat+det}}\rangle/\langle A^{2}_{+,{ LR,stat+det}}\rangle$, separately for the $\eta>0$ and $\eta<0$ regions. The $\phi$-acceptance correction was applied for the results in this figure.
Left panel: Statistical fluctuation and detector effects in the charge asymmetry variance (multiplied by the number of participants $N_{part}$) from the $\eta<0$ region. The dotted curve shows the $1/N$ approximation, the dashed curve shows the statistical fluctuations $\langle A^{2}_{-,{ LR,stat}}\rangle$ obtained by the (50-50) method (see the text). The solid curve connecting the solid points shows the net effect of the statistical fluctuations and detector non-uniformities, $\langle A^{2}_{-,{ LR,stat+det}}\rangle$, obtained by the adding-$\pi$ method, and the crosses shows the same but obtained from the ``scramble'' method. See the text for details. Middle panel: The statistical fluctuation effects relative to the $1/N$ approximation (thin curves) and the effects due to the imperfect detector (thick curves). The dashed curves are for the region $\eta>0$ and the solid curves are for $\eta<0$. Right panel: The ratios of the statistical fluctuation and detector effects $\langle A^{2}_{+,{ LR,stat+det}}\rangle/\langle A^{2}_{-,{ LR,stat+det}}\rangle$ and $\langle A^{2}_{+,{ UD,stat+det}}\rangle/\langle A^{2}_{+,{ LR,stat+det}}\rangle$, separately for the $\eta>0$ and $\eta<0$ regions. The $\phi$-acceptance correction was applied for the results in this figure.
Left panel: Statistical fluctuation and detector effects in the charge asymmetry variance (multiplied by the number of participants $N_{part}$) from the $\eta<0$ region. The dotted curve shows the $1/N$ approximation, the dashed curve shows the statistical fluctuations $\langle A^{2}_{-,{ LR,stat}}\rangle$ obtained by the (50-50) method (see the text). The solid curve connecting the solid points shows the net effect of the statistical fluctuations and detector non-uniformities, $\langle A^{2}_{-,{ LR,stat+det}}\rangle$, obtained by the adding-$\pi$ method, and the crosses shows the same but obtained from the ``scramble'' method. See the text for details. Middle panel: The statistical fluctuation effects relative to the $1/N$ approximation (thin curves) and the effects due to the imperfect detector (thick curves). The dashed curves are for the region $\eta>0$ and the solid curves are for $\eta<0$. Right panel: The ratios of the statistical fluctuation and detector effects $\langle A^{2}_{+,{ LR,stat+det}}\rangle/\langle A^{2}_{-,{ LR,stat+det}}\rangle$ and $\langle A^{2}_{+,{ UD,stat+det}}\rangle/\langle A^{2}_{+,{ LR,stat+det}}\rangle$, separately for the $\eta>0$ and $\eta<0$ regions. The $\phi$-acceptance correction was applied for the results in this figure.
The asymmetry correlations, $\langle A^{2}_{+,{ UD}}\rangle$ (left panel), $\langle A^{2}_{-,{ UD}}\rangle$ (middle panel), and $\langle A_{+}A_{-}\rangle_{ UD}$ (right panel), multiplied by the number of participants $N_{part}$, separately for $\eta>0$ and $\eta<0$. The star and triangle depict the results from $d$+Au collisions. The net effects of the statistical fluctuations and detector non-uniformities are shown as the curves.
The asymmetry correlations, $\langle A^{2}_{+,{ UD}}\rangle$ (left panel), $\langle A^{2}_{-,{ UD}}\rangle$ (middle panel), and $\langle A_{+}A_{-}\rangle_{ UD}$ (right panel), multiplied by the number of participants $N_{part}$, separately for $\eta>0$ and $\eta<0$. The star and triangle depict the results from $d$+Au collisions. The net effects of the statistical fluctuations and detector non-uniformities are shown as the curves.
The asymmetry correlations, $\langle A^{2}_{+,{ UD}}\rangle$ (left panel), $\langle A^{2}_{-,{ UD}}\rangle$ (middle panel), and $\langle A_{+}A_{-}\rangle_{ UD}$ (right panel), multiplied by the number of participants $N_{part}$, separately for $\eta>0$ and $\eta<0$. The star and triangle depict the results from $d$+Au collisions. The net effects of the statistical fluctuations and detector non-uniformities are shown as the curves.
The statistical and detector effect subtracted asymmetry correlations, $\delta\langle A^{2}_{+,0^{\circ}\pm\Delta\phi_{w}}\rangle$ (left panel), $\delta\langle A^{2}_{-,0^{\circ}\pm\Delta\phi_{w}}\rangle$ (middle panel), and $\delta\langle A_{+}A_{-}\rangle_{ LR}$ (right panel), multiplied by the number of participants $N_{part}$, before and after the corrections for the $\phi$-dependent acceptance $\times$ efficiency.
The statistical and detector effect subtracted asymmetry correlations, $\delta\langle A^{2}_{+,0^{\circ}\pm\Delta\phi_{w}}\rangle$ (left panel), $\delta\langle A^{2}_{-,0^{\circ}\pm\Delta\phi_{w}}\rangle$ (middle panel), and $\delta\langle A_{+}A_{-}\rangle_{ LR}$ (right panel), multiplied by the number of participants $N_{part}$, before and after the corrections for the $\phi$-dependent acceptance $\times$ efficiency.
The statistical and detector effect subtracted asymmetry correlations, $\delta\langle A^{2}_{+,0^{\circ}\pm\Delta\phi_{w}}\rangle$ (left panel), $\delta\langle A^{2}_{-,0^{\circ}\pm\Delta\phi_{w}}\rangle$ (middle panel), and $\delta\langle A_{+}A_{-}\rangle_{ LR}$ (right panel), multiplied by the number of participants $N_{part}$, before and after the corrections for the $\phi$-dependent acceptance $\times$ efficiency.
Dynamical charge asymmetry variance after removing the statistical and detector effects, $\delta\langle A^{2}_{\pm,{ LR}}\rangle=\langle A^{2}_{\pm,{ LR}}\rangle-\langle A^{2}_{\pm,{ LR,stat+det}}\rangle$, scaled by the number of participants $N_{part}$. The results are consistent between positive and negative $\eta$ regions and between positive and negative charges.
The second-harmonic event-plane resolution of sub-events ($\eta<0$ and $\eta>0$) as a function of the number of participants.
Charge multiplicity asymmetry correlations, $\delta\langle A^{2}\rangle$ (left panel) and $\delta\langle A_{+}A_{-}\rangle$ (middle panel), and their differences between UD\ and LR\ (right panel) as a function of the event-plane resolution $\epsilon_{ EP}(f)=\sqrt{\mean{\cos2(\psi_{{ EP},\eta>0}(f)-\psi_{{ EP},\eta<0}(f))}}$ in 20-30% central Au+Au collisions. The solid lines are free linear fits to the data, while the dashed lines are linear fits with the intercept fixed to zero at $\epsilon_{ EP}(f)=0$.
Charge multiplicity asymmetry correlations, $\delta\langle A^{2}\rangle$ (left panel) and $\delta\langle A_{+}A_{-}\rangle$ (middle panel), and their differences between UD\ and LR\ (right panel) as a function of the event-plane resolution $\epsilon_{ EP}(f)=\sqrt{\mean{\cos2(\psi_{{ EP},\eta>0}(f)-\psi_{{ EP},\eta<0}(f))}}$ in 20-30% central Au+Au collisions. The solid lines are free linear fits to the data, while the dashed lines are linear fits with the intercept fixed to zero at $\epsilon_{ EP}(f)=0$.
TCharge multiplicity asymmetry correlations, $\delta\langle A^{2}\rangle$ (left panel) and $\delta\langle A_{+}A_{-}\rangle$ (middle panel), and their differences between UD\ and LR\ (right panel) as a function of the event-plane resolution $\epsilon_{ EP}(f)=\sqrt{\mean{\cos2(\psi_{{ EP},\eta>0}(f)-\psi_{{ EP},\eta<0}(f))}}$ in 20-30% central Au+Au collisions. The solid lines are free linear fits to the data, while the dashed lines are linear fits with the intercept fixed to zero at $\epsilon_{ EP}(f)=0$.
The TPC second-harmonic (upper left) and ZDC-SMD first harmonic (upper right) event-plane resolution as a function of $v^{obs}_{2}$ in 20-40% central Au+Au collisions. The TPC second-harmonic (lower left) and ZDC-SMD first harmonic (lower right) event-plane resolution for events with $|v^{obs}_{2}|<0.04$ as a function of centrality.
The TPC second-harmonic (upper left) and ZDC-SMD first harmonic (upper right) event-plane resolution as a function of $v^{obs}_{2}$ in 20-40% central Au+Au collisions. The TPC second-harmonic (lower left) and ZDC-SMD first harmonic (lower right) event-plane resolution for events with $|v^{obs}_{2}|<0.04$ as a function of centrality.
The TPC second-harmonic (upper left) and ZDC-SMD first harmonic (upper right) event-plane resolution as a function of $v^{obs}_{2}$ in 20-40% central Au+Au collisions. The TPC second-harmonic (lower left) and ZDC-SMD first harmonic (lower right) event-plane resolution for events with $|v^{obs}_{2}|<0.04$ as a function of centrality.
The TPC second-harmonic (upper left) and ZDC-SMD first harmonic (upper right) event-plane resolution as a function of $v^{obs}_{2}$ in 20-40% central Au+Au collisions. The TPC second-harmonic (lower left) and ZDC-SMD first harmonic (lower right) event-plane resolution for events with $|v^{obs}_{2}|<0.04$ as a function of centrality.
Dihadron azimuthal correlations containing a high transverse momentum ($p_T$) trigger particle are sensitive to the properties of the nuclear medium created at RHIC through the strong interactions occurring between the traversing parton and the medium, i.e. jet-quenching. Previous measurements revealed a strong modification to dihadron azimuthal correlations in Au+Au collisions with respect to p+p and d+Au collisions. The modification increases with the collision centrality, suggesting a path-length or energy density dependence to the jet-quenching effect. This paper reports STAR measurements of dihadron azimuthal correlations in mid-central (20-60%) Au+Au collisions at $\sqrt{s_{_{\rm NN}}}=200$ GeV as a function of the trigger particle's azimuthal angle relative to the event plane, $\phi_s=|\phi_t-\psi_{\rm EP}|$. The azimuthal correlation is studied as a function of both the trigger and associated particle $p_T$. The subtractions of the combinatorial background and anisotropic flow, assuming Zero Yield At Minimum (ZYAM), are described. The correlation results are first discussed with subtraction of the even harmonic (elliptic and quadrangular) flow backgrounds. The away-side correlation is strongly modified, and the modification varies with $\phi_s$, with a double-peak structure for out-of-plane trigger particles. The near-side ridge (long range pseudo-rapidity $\Delta\eta$ correlation) appears to drop with increasing $\phi_s$ while the jet-like component remains approximately constant. The correlation functions are further studied with subtraction of odd harmonic triangular flow background arising from fluctuations. It is found that the triangular flow, while responsible for the majority of the amplitudes, is not sufficient to explain the $\phi_s$-dependence of the ridge or the away-side double-peak structure. ...
red data points
black histogram
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
dN/deta phis=045 deg, pt=0.151 GeV/c
dN/deta phis=045 deg, pt=0.153 GeV/c
dN/deta phis=090 deg, pt=0.51 GeV/c
dN/deta phis=090 deg, pt=12 GeV/c
dN/deta phis=4590 deg, pt=0.151 GeV/c
sigma vs phis pt=0.151 GeV/c
sigma vs phis pt=0.153 GeV/c
sigma vs phis pt=0.51 GeV/c
sigma vs phis pt=12 GeV/c
sigma vs pt phis=045 deg
sigma vs pt phis=090 deg
sigma vs pt phis=4590 deg
background uncertainty caps in the figure
flow uncertainty curves in the figure
leadage uncertainty arrows in the figure
total uncertainty boxes in the figure
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
0^{o} < phi_{s} < 45^{o}
45^{o} < phi_{s} < 90^{o}
Previous in-plane result published in 2004
Previous out-of-plane result published in 2004
3<p_{\text{T}}^{(t)}<4, 1<p_{\text{T}}^{(a)}<2 GeV/c, 0^{o} < phi_{s} < 45^{o}
3<p_{\text{T}}^{(t)}<4, 1<p_{\text{T}}^{(a)}<2 GeV/c, 45^{o} < phi_{s} < 90^{o}
3<p_{\text{T}}^{(t)}<4, 2<p_{\text{T}}^{(a)}<3 GeV/c, 0^{o} < phi_{s} < 45^{o}
3<p_{\text{T}}^{(t)}<4, 2<p_{\text{T}}^{(a)}<3 GeV/c, 45^{o} < phi_{s} < 90^{o}
4<p_{\text{T}}^{(t)}<6, 1<p_{\text{T}}^{(a)}<2 GeV/c, 0^{o} < phi_{s} < 45^{o}
4<p_{\text{T}}^{(t)}<6, 1<p_{\text{T}}^{(a)}<2 GeV/c, 45^{o} < phi_{s} < 90^{o}
4<p_{\text{T}}^{(t)}<6, 2<p_{\text{T}}^{(a)}<3 GeV/c, 0^{o} < phi_{s} < 45^{o}
4<p_{\text{T}}^{(t)}<6, 2<p_{\text{T}}^{(a)}<3 GeV/c, 45^{o} < phi_{s} < 90^{o}
3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
3<p_{\text{T}}^{(t)}<4 GeV/c
3<p_{\text{T}}^{(t)}<4 GeV/c, 0^{o}15^{o}
3<p_{\text{T}}^{(t)}<4 GeV/c, 75^{o}90^{o}
Cone region, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
one region, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
one region, 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
one region, 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
i region, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
Pi region, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
i region, 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
i region, 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
d+Au, 3<p_{\text{T}}^{(t)}<4 GeV/c
20-60%, 3<p_{T}^{(t)}<4 GeV/c, (a) 0^{o}<#phi_{s}<15^{o}
20-60%, 3<p_{T}^{(t)}<4 GeV/c, (b) 75^{o}<#phi_{s}<90^{o}
20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, (a) 0^{o}<phi_{s}<15^{o}
20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, (b) 75^{o}<phi_{s}<90^{o}
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 0, jet
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 1, jet
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 2, jet
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 3, jet
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 4, jet
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 5, jet
1<p_{\text{T}}^{(a)}<2 GeV/c, jet
0-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/, slice 0, ridge
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 1, ridge
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 2, ridge
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 3, ridge
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 4, ridge
20-60% Au+Au, 3<p_{T}^{(t)}<4 GeV/c, 1<p_{T}^{(a)}<2 GeV/c, slice 5, ridge
1<p_{\text{T}}^{(a)}<2 GeV/c, ridge
jet (Deltaphi|<1.0, |Deltaeta|<0.7) 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
jet (Deltaphi|<1.0, |Deltaeta|<0.7) 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
ridge (Deltaphi|<1.0, |Deltaeta|>0.7) 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
ridge (Deltaphi|<1.0, |Deltaeta|>0.7) 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
ridge (Deltaphi|<1.0, |Deltaeta|>0.7) 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
ridge (Deltaphi|<1.0, |Deltaeta|>0.7) 4<p_{\text{T}}^{(t)}<6 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
3<p_{\text{T}}^{(t)}<4 GeV/c Ridge (75^{o}<|phi_{s}|<90^{o}) / Ridge (0^{o}<|phi_{s}|<15^{o})
4<p_{\text{T}}^{(t)}<6 GeV/c Ridge (75^{o}<|phi_{s}|<90^{o}) / Ridge (0^{o}<|phi_{s}|<15^{o})
3<p_{\text{T}}^{(t)}<4 GeV/c Ridge (30^{o}<|phi_{s}|<45^{o}) / Ridge (0^{o}<|phi_{s}|<15^{o})
4<p_{\text{T}}^{(t)}<6 GeV/c Ridge (30^{o}<|phi_{s}|<45^{o}) / Ridge (0^{o}<|phi_{s}|<15^{o})
3<p_{\text{T}}^{(t)}<4 GeV/c Ridge (0^{o}<|phi_{s}|<15^{o}) / Jet (0^{o}<|phi_{s}|<15^{o})
4<p_{\text{T}}^{(t)}<6 GeV/c Ridge (0^{o}<|phi_{s}|<15^{o}) / Jet (0^{o}<|phi_{s}|<15^{o})
3<p_{\text{T}}^{(t)}<4 GeV/c, cone region
4<p_{\text{T}}^{(t)}<6 GeV/c, cone region
3<p_{\text{T}}^{(t)}<4 GeV/c, jetlike
4<p_{\text{T}}^{(t)}<6 GeV/c, jetlike
3<p_{\text{T}}^{(t)}<4 GeV/c, pi region
4<p_{\text{T}}^{(t)}<6 GeV/c, pi region
3<p_{\text{T}}^{(t)}<4 GeV/c, ridge
4<p_{\text{T}}^{(t)}<6 GeV/c, ridge
fig17_ampl_pt_inclusive
3<p_{\text{T}}^{(t)}<4 GeV/c, 0^{o}<phi_{s}<45^{o}, cone region
3<p_{\text{T}}^{(t)}<4 GeV/c, 0^{o}<phi_{s}<45^{o}, jetlike
3<p_{\text{T}}^{(t)}<4 GeV/c, 0^{o}<phi_{s}<45^{o}, pi region
3<p_{\text{T}}^{(t)}<4 GeV/c, 0^{o}<phi_{s}<45^{o}, pi region ridge
3<p_{\text{T}}^{(t)}<4 GeV/c, 0^{o}<phi_{s}<45^{o}, ridge
3<p_{\text{T}}^{(t)}<4 GeV/c, 45^{o}<phi_{s}<90^{o}, cone region
3<p_{\text{T}}^{(t)}<4 GeV/c, 45^{o}<phi_{s}<90^{o}, jetlike
3<p_{\text{T}}^{(t)}<4 GeV/c, 45^{o}<phi_{s}<90^{o}, pi region
3<p_{\text{T}}^{(t)}<4 GeV/c, 45^{o}<phi_{s}<90^{o}, pi region ridge
3<p_{\text{T}}^{(t)}<4 GeV/c, 45^{o}<phi_{s}<90^{o}, ridge
4<p_{\text{T}}^{(t)}<6 GeV/c, 0^{o}<phi_{s}<45^{o}, cone region
4<p_{\text{T}}^{(t)}<6 GeV/c, 0^{o}<phi_{s}<45^{o}, jetlike
4<p_{\text{T}}^{(t)}<6 GeV/c, 0^{o}<phi_{s}<45^{o}, pi region
4<p_{\text{T}}^{(t)}<6 GeV/c, 0^{o}<phi_{s}<45^{o}, pi region ridge
4<p_{\text{T}}^{(t)}<6 GeV/c, 0^{o}<phi_{s}<45^{o}, ridge
4<p_{\text{T}}^{(t)}<6 GeV/c, 45^{o}<phi_{s}<90^{o}, cone region
4<p_{\text{T}}^{(t)}<6 GeV/c, 45^{o}<phi_{s}<90^{o}, jetlike
4<p_{\text{T}}^{(t)}<6 GeV/c, 45^{o}<phi_{s}<90^{o}, pi region
4<p_{\text{T}}^{(t)}<6 GeV/c, 45^{o}<phi_{s}<90^{o}, pi region ridge
4<p_{\text{T}}^{(t)}<6 GeV/c, 45^{o}<phi_{s}<90^{o}, ridge
jetlike eta sigma
cone peak phi sigma
jetlike phi sigma
ridge phi sigma
jetlike eta sigma
cone peak phi sigma
jetlike phi sigma
ridge phi sigma
dAu jetlike eta sigma
dAu jetlike phi sigma
cone peak centroid
cone peak centroid
cone peak centroid
cone peak centroid
cone peak centroid
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
v_{2} /3
v_{3}
v_{4}
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c, slice 5
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 0
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 1
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 2
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 3
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c, slice 5
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, 2<p_{\text{T}}^{(a)}<4 GeV/c
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, 1<p_{\text{T}}^{(a)}<2 GeV/c
background subtracted correlation with upper flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 0
background subtracted correlation with upper flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 1
background subtracted correlation with upper flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 2
background subtracted correlation with upper flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 3
background subtracted correlation with upper flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 4
background subtracted correlation with upper flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 5
background subtracted correlation with upper flow systematic uncertainty Difference of the above results default results in Fig.21, slice 0
background subtracted correlation with upper flow systematic uncertainty Difference of the above results default results in Fig.21, slice 1
background subtracted correlation with upper flow systematic uncertainty Difference of the above results default results in Fig.21, slice 2
background subtracted correlation with upper flow systematic uncertainty Difference of the above results default results in Fig.21, slice 3
background subtracted correlation with upper flow systematic uncertainty Difference of the above results default results in Fig.21, slice 4
background subtracted correlation with upper flow systematic uncertainty Difference of the above results default results in Fig.21, slice 5
background subtracted correlation with lower flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 0
background subtracted correlation with lower flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 1
background subtracted correlation with lower flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 2
background subtracted correlation with lower flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 3
background subtracted correlation with lower flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 4
background subtracted correlation with lower flow systematic uncertainty EP^{ } include |Deltaeta|<0.5 particles, slice 5
background subtracted correlation with lower flow systematic uncertainty Difference of the above results default results in Fig.21, slice 0
background subtracted correlation with lower flow systematic uncertainty Difference of the above results default results in Fig.21, slice 1
background subtracted correlation with lower flow systematic uncertainty Difference of the above results default results in Fig.21, slice 2
background subtracted correlation with lower flow systematic uncertainty Difference of the above results default results in Fig.21, slice 3
background subtracted correlation with lower flow systematic uncertainty Difference of the above results default results in Fig.21, slice 4
background subtracted correlation with lower flow systematic uncertainty Difference of the above results default results in Fig.21, slice 5
background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles, slice 0
background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles, slice 1
background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles, slice 2
background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles, slice 3
background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles, slice 4
background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles, slice 5
background subtracted correlation Difference of the above results default results in Fig.21, slice 0
background subtracted correlation Difference of the above results default results in Fig.21, slice 1
background subtracted correlation Difference of the above results default results in Fig.21, slice 2
background subtracted correlation Difference of the above results default results in Fig.21, slice 3
background subtracted correlation Difference of the above results default results in Fig.21, slice 4
background subtracted correlation Difference of the above results default results in Fig.21, slice 5
d+Au background subtracted correlation EP^{ } include |Deltaeta|<0.5 particles
difference from default results, slice 0
difference from default results, slice 1
difference from default results, slice 2
difference from default results, slice 3
difference from default results, slice 4
difference from default results, slice 5
raw signal
bkgd <v2t*v2>
bkgd <v2t>*<v2> (previous inclusive analysis)
bkgd <v2t*v2> subtracted
bkgd <v2t>*<v2> subtracted (previous inclusive analysis)
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
d+Au raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
d+Au raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
d+Au raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
d+Au raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
d+Au raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with default flow Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
flow background with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 2
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 3
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 4
raw correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 5
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 0
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background normalization systematic uncertainty band Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 3
background normalization systematic uncertainty band 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 4
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, slice 1
background normalization systematic uncertainty band 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 5
background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, slice 1
background normalization systematic uncertainty band 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 4
background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 4
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 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 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 3
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%, 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 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 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 0
d+Au background subtracted correlation Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7, slice 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 5
d+Au background subtracted correlation Au+Au 20-60%, 3<p_{\text{T}}^{(t)}<4 GeV/c, |Deltaeta|>0.7
background subtracted correlation with upper flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 0
background subtracted correlation with lower flow systematic uncertainty Au+Au 20-60%, 4<p_{\text{T}}^{(t)}<6 GeV/c, |Deltaeta|>0.7, slice 1
Quark interactions with topological gluon configurations can induce chirality imbalance and local parity violation in quantum chromodynamics. This can lead to electric charge separation along the strong magnetic field in relativistic heavy-ion collisions -- the chiral magnetic effect (CME). We report measurements by the STAR collaboration of a CME-sensitive observable in $p$+Au and $d$+Au collisions at 200 GeV, where the CME is not expected, using charge-dependent pair correlations relative to a third particle. We observe strong charge-dependent correlations similar to those measured in heavy-ion collisions. This bears important implications for the interpretation of the heavy-ion data.
When you search on a word, e.g. 'collisions', we will automatically search across everything we store about a record. But sometimes you may wish to be more specific. Here we show you how.
Guidance on the query string syntax can also be found in the OpenSearch documentation.
About HEPData Submitting to HEPData HEPData File Formats HEPData Coordinators HEPData Terms of Use HEPData Cookie Policy
Status
Email
Forum
Twitter
GitHub
Copyright ~1975-Present, HEPData | Powered by Invenio, funded by STFC, hosted and originally developed at CERN, supported and further developed at IPPP Durham.