'Identified transverse momentum spectra of $\pi^{-}$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV'

'Identified transverse momentum spectra of $K^{-}$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV'

'Identified transverse momentum spectra of $\bar{p}$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV'

'Average transverse momentum as a function of $\langle$N$_{part}$$\rangle$ for $\pi^{+}$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

'Average transverse momentum as a function of $\langle$N$_{part}$$\rangle$ for $K^{+}$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

'Average transverse momentum as a function of $\langle$N$_{part}$$\rangle$ for p at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

'dN/dy scaled by 0.5 × $\langle$N$_{part}$$\rangle$ as a function of $\langle$N$_{part}$$\rangle$ for $\pi^{+}$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

'dN/dy scaled by 0.5 × $\langle$N$_{part}$$\rangle$ as a function of $\langle$N$_{part}$$\rangle$ for $K^{+}$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

'dN/dy scaled by 0.5 × $\langle$N$_{part}$$\rangle$ as a function of $\langle$N$_{part}$$\rangle$ for p at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

'dN/dy scaled by 0.5 × $\langle$N$_{part}$$\rangle$ as a function of $\langle$N$_{part}$$\rangle$ for $\bar{p}$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

'$\pi^{−}$/$\pi^{+}$ ratio as a function of $\langle$N$_{part}$$\rangle$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

'$K^{−}$/$K^{+}$ ratio as a function of $\langle$N$_{part}$$\rangle$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

'$\bar{p}$/p ratio as a function of $\langle$N$_{part}$$\rangle$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

'$K^{+}$/$\pi^{+}$ ratio as a function of $\langle$N$_{part}$$\rangle$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

'$K^{-}$/$\pi^{-}$ ratio as a function of $\langle$N$_{part}$$\rangle$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

'p/$\pi^{+}$ ratio as a function of $\langle$N$_{part}$$\rangle$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

'$\bar{p}$/$\pi^{-}$ ratio as a function of $\langle$N$_{part}$$\rangle$ at midrapidity (|y| < 0.1) in U+U collisions at $\sqrt{s_{\rm NN}}$ = 193 GeV.'

The Au+Au 200 GeV measurements of the two-, four- and six-particle elliptic flow and the elliptic flow fluctuations.

The Au+Au 54.4 GeV measurements of the two-, four- and six-particle elliptic flow and the elliptic flow fluctuations.

The Au+Au 39 GeV measurements of the two-, four- and six-particle elliptic flow and the elliptic flow fluctuations.

The Au+Au 27 GeV measurements of the two-, four- and six-particle elliptic flow and the elliptic flow fluctuations.

The Au+Au 19.6 GeV measurements of the two- and four-particle elliptic flow and the elliptic flow fluctuations.

The Au+Au 11.5 GeV measurements of the two- and four-particle elliptic flow and the elliptic flow fluctuations.

The U+U 193 GeV measurements of the two-, four- and six-particle elliptic flow and the elliptic flow fluctuations.

The Cu+Au 200 GeV measurements of the two-, four- and six-particle elliptic flow and the elliptic flow fluctuations.

The $p_{\text{T}}$ dependence of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The $p_{\text{T}}$ dependence of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The $p_{\text{T}}$ dependence of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The $p_{\text{T}}$ dependence of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The $p_{\text{T}}$ dependence of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The $p_{\text{T}}$ dependence of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The $p_{\text{T}}$ dependence of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The $p_{\text{T}}$ dependence of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The $p_{\text{T}}$ dependence of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The $p_{\text{T}}$ dependence of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The $p_{\text{T}}$ dependence of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The $p_{\text{T}}$ dependence of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The $p_{\text{T}}$ dependence of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV for different centrality classes. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Flow coefficients $v_{n}$ as a function of transverse kinetic energy $KE_{\text{T}}/n_{q}$ for various particles at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

The flow coefficients $v_{n}$ scaled by $\varepsilon_{n}\left\lbrace 2\right\rbrace$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified particles versus $(m_{T}-m_{0})/n_{q}$ for three centrality bins in U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. The error bars represent statistical uncertainties. The bands represent point-by-point systematic uncertainties.

Ratios of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1.0) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. Error bars represent statistical uncertainties.

Ratios of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1.0) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. Error bars represent statistical uncertainties.

Ratios of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1.0) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. Error bars represent statistical uncertainties.

Ratios of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1.0) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. Error bars represent statistical uncertainties.

Ratios of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1.0) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. Error bars represent statistical uncertainties.

Ratios of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1.0) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. Error bars represent statistical uncertainties.

Ratios of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1.0) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. Error bars represent statistical uncertainties.

Ratios of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1.0) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. Error bars represent statistical uncertainties.

Ratios of $v_{n}$ coefficients at mid-rapidity ($|y| <$ 1.0) in minimum bias U+U collisions at $\sqrt{s_{NN}}$ = 193 GeV. Error bars represent statistical uncertainties.

Differential cross section for DIS events as a function of Q**2.

Differential cross section for DIS events as a function of ET_jet1.

Differential cross section for DIS events as a function of mean(ETARAP_jets).

Differential cross section for DIS events as a function of DIFF(ETARAP_jets).

Differential cross section for photoproduction events as a function of Z_Pomeron.

Differential cross section for photoproduction events as a function of X_=Gamma.

Differential cross section for photoproduction events as a function of LOG10(X_Pomeron).

Differential cross section for photoproduction events as a function of W.

Differential cross section for photoproduction events as a function of ET_jet1.

Differential cross section for photoproduction events as a function of MEAN(ETARAP_jets).

Differential cross section for photoproduction events as a function of DIFF(ETARAP_jets).

Differential cross section for photoproduction events as a function of M(jets).

Cross section for elastic J/PSI photoproduction as a function of W in Q**2 bins for ABS(T) < 1.2 GeV**2.

Cross section for elastic J/PSI photoproduction as a function of W in Q**2 bins for ABS(T) < 1.2 GeV**2.

Parameters of the fits of the cross section as W**POWER and slope of the D(SIG)/DT distribution.

Differential cross section for the elastic process GAMMA P --> J/PSI P as a function of T in Q**2 bins in the W range 40 to 160 GeV.

Differential cross section for the elastic process GAMMA P --> J/PSI P as a function of T in Q**2 bins in the W range 40 to 160 GeV.

Differential cross section for the elastic process GAMMA P --> J/PSI P as a function of T in Q**2 bins in the W range 40 to 160 GeV.

Differential cross section for the elastic process GAMMA P --> J/PSI P as a function of T in Q**2 bins in the W range 40 to 160 GeV.

Differential photoproduction cross section for the elastic process GAMMA P --> J/PSI P as a function of W in bins of ABS(T).

Differential electroproduction cross section for the elastic process GAMMA P --> J/PSI P as a function of W in bins of ABS(T).

Slope parameter derived from the one dimensional fit to the DSIG/DT differential distribution as a function of W in Q**2 bins in the electroproduction region.

Slope parameter derived from the one dimensional fit to the DSIG/DT differential distribution as a function of W in Q**2 bins in the photoproduction region.

Spin density matrices and ratio R of cross sections of longitudinal and polarized photons as a function of Q**2 for ABS(T) < 5 GeV**2 and W from 40 to 160 GeV.

Spin density matrices as a function of Q**2 for ABS(T) < 5 GeV**2 and W from 40 to 160 GeV.

Spin density matrix elements as a function of ABS(T) for photoproduction data in the W region 40 to 160 GeV.

Spin density matrix elements as a function of ABS(T) for electroproduction data in the W region 40 to 160 GeV.

Spin density matrix elements as a function of ABS(T) in the W range 40 to 160 GeV for the electroproduction region.

Differential cross sections for non-radiative E+ E- --> E+ E- events at centre of mass energy 196 GeV.

Differential cross sections for non-radiative E+ E- --> E+ E- events at centre of mass energy 200 GeV.

Differential cross sections for non-radiative E+ E- --> E+ E- events at centre of mass energy 202 GeV.

Differential cross sections for non-radiative E+ E- --> E+ E- events at centre of mass energy 205 GeV.

Differential cross sections for non-radiative E+ E- --> E+ E- events at centre of mass energy 207 GeV.

Measured cross sections and forward-backward asymmetries for inclusive E+ E- --> MU+ MU- events.

Measured cross sections and forward-backward asymmetries for non-radiative E+ E- --> MU+ MU- events.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 183 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 189 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 192 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 196 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 200 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 202 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 205 GeV.

Differential cross sections for non-radiative E+ E- --> MU+ MU- events at centre of mass energy 207 GeV.

Measured cross sections and forward-backward asymmetries for inclusive E+ E- --> TAU+ TAU- events.

Measured cross sections and forward-backward asymmetries for non-radiative E+ E- --> TAU+ TAU- events.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 183 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 189 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 192 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 196 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 200 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 202 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 205 GeV.

Differential cross sections for non-radiative E+ E- --> TAU+ TAU- events atcentre of mass energy 207 GeV.

Measured values of the inclusive and non radiative cross sections for the process E+ E- --> Q QBAR.

Total cross section for MU+ MU- and HADRON production in the defined kinematic range. Corrections for detector effects based on BDKRC (for MU+ MU-) and PYTHIA and TWOGAM (for hadrons) event generators.

W pair production cross section for all channels.

W- polar angle differential cross sections from the semi-leptonic decay mode. The first and second systematic errors (DSYS) are due to the background and efficiency uncertainties respectively.