• Browse all
Azimuthal anisotropy measurements of strange and multi-strange hadrons in U+U collisions at $\sqrt{s_{NN}} = 193$ GeV at RHIC

The collaboration
2021.

Abstract (data abstract)
No description provided.

• #### Event Plane Resolution, U+U 193 GeV

10.17182/hepdata.102643.v1/t1

Event plane resolution as a function of centrality for $\psi_{2}$, $\psi_{3}$, and $\psi_{4}$ in U+U collisions at $\sqrt{s_{NN}}$ = 193...

• #### $K^{0}_{s}$ $v_{2}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t2

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...

• #### $\phi$ $v_{2}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t3

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...

• #### $\Lambda$ $v_{2}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t4

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...

• #### $\Xi$ $v_{2}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t5

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...

• #### $\Omega$ $v_{2}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t6

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...

• #### $K^{0}_{s}$ $v_{3}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t7

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...

• #### $\phi$ $v_{3}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t8

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...

• #### $\Lambda$ $v_{3}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t9

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...

• #### $\Xi$ $v_{3}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t10

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...

• #### $\Omega$ $v_{3}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t11

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...

• #### $K^{0}_{s}$ $v_{4}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t12

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...

• #### $\phi$ $v_{4}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t13

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...

• #### $\Lambda$ $v_{4}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t14

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...

• #### $\Xi$ $v_{4}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t15

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...

• #### $\Omega$ $v_{4}$($p_{\text{T}}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t16

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...

• #### $K^{0}_{s}$ $v_{2}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t17

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $K^{0}_{s}$ $v_{2}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t18

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $K^{0}_{s}$ $v_{2}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t19

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\phi$ $v_{2}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t20

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\phi$ $v_{2}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t21

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\phi$ $v_{2}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t22

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Lambda$ $v_{2}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t23

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Lambda$ $v_{2}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t24

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Lambda$ $v_{2}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t25

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Xi$ $v_{2}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t26

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Xi$ $v_{2}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t27

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Xi$ $v_{2}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t28

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Omega$ $v_{2}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t29

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Omega$ $v_{2}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t30

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Omega$ $v_{2}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t31

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $K^{0}_{s}$ $v_{3}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t32

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $K^{0}_{s}$ $v_{3}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t33

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $K^{0}_{s}$ $v_{3}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t34

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\phi$ $v_{3}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t35

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\phi$ $v_{3}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t36

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\phi$ $v_{3}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t37

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Lambda$ $v_{3}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t38

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Lambda$ $v_{3}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t39

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Lambda$ $v_{3}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t40

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Xi$ $v_{3}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t41

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Xi$ $v_{3}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t42

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Xi$ $v_{3}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t43

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Omega$ $v_{3}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t44

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Omega$ $v_{3}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t45

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $K^{0}_{s}$ $v_{4}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t46

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $K^{0}_{s}$ $v_{4}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t47

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $K^{0}_{s}$ $v_{4}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t48

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\phi$ $v_{4}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t49

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\phi$ $v_{4}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t50

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Lambda$ $v_{4}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t51

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Lambda$ $v_{4}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t52

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Lambda$ $v_{4}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t53

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Xi$ $v_{4}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t54

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Xi$ $v_{4}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t55

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $\Omega$ $v_{4}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t56

The flow coefficients $v_{n}$ as a function of $p_{\text{T}}$ at mid-rapidity ($|y| <$ 1) in U+U collisions at $\sqrt{s_{NN}}$ =...

• #### $K^{0}_{s}$ $v_{2}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t57

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...

• #### $\phi$ $v_{2}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t58

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...

• #### $\Lambda$ $v_{2}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t59

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...

• #### $\Xi$ $v_{2}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t60

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...

• #### $\Omega$ $v_{2}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t61

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...

• #### $K^{0}_{s}$ $v_{3}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t62

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...

• #### $\phi$ $v_{3}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t63

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...

• #### $\Lambda$ $v_{3}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t64

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...

• #### $\Xi$ $v_{3}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t65

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...

• #### $\Omega$ $v_{3}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t66

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...

• #### $K^{0}_{s}$ $v_{4}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t67

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...

• #### $\phi$ $v_{4}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t68

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...

• #### $\Lambda$ $v_{4}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t69

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...

• #### $\Xi$ $v_{4}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t70

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...

• #### $\Omega$ $v_{4}/n_{q}$($KE_{T}/n_{q}$), Centrality 0-80%

10.17182/hepdata.102643.v1/t71

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...

• #### $K^{0}_{s}$ $v_{2}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t72

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...

• #### $\phi$ $v_{2}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t73

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...

• #### $\Lambda$ $v_{2}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t74

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...

• #### $\Xi$ $v_{2}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t75

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...

• #### $\Omega$ $v_{2}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t76

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...

• #### $K^{0}_{s}$ $v_{3}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t77

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...

• #### $\phi$ $v_{3}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t78

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...

• #### $\Lambda$ $v_{3}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t79

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...

• #### $\Xi$ $v_{3}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t80

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...

• #### $\Omega$ $v_{3}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t81

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...

• #### $K^{0}_{s}$ $v_{4}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t82

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...

• #### $\phi$ $v_{4}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t83

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...

• #### $\Lambda$ $v_{4}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t84

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...

• #### $\Xi$ $v_{4}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t85

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...

• #### $\Omega$ $v_{4}/n_{q}$($KE_{T}/n_{q}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t86

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...

• #### $K^{0}_{s}$ $v_{2}/e_{2}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t87

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...

• #### $\phi$ $v_{2}/e_{2}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t88

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...

• #### $\Lambda$ $v_{2}/e_{2}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t89

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...

• #### $\Xi$ $v_{2}/e_{2}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t90

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...

• #### $K^{0}_{s}$ $v_{2}/e_{2}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t91

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...

• #### $\phi$ $v_{2}/e_{2}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t92

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...

• #### $\Lambda$ $v_{2}/e_{2}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t93

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...

• #### $\Xi$ $v_{2}/e_{2}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t94

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...

• #### $K^{0}_{s}$ $v_{2}/e_{2}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t95

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...

• #### $\phi$ $v_{2}/e_{2}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t96

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...

• #### $\Lambda$ $v_{2}/e_{2}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t97

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...

• #### $\Xi$ $v_{2}/e_{2}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t98

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...

• #### $K^{0}_{s}$ $v_{3}/e_{3}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t99

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...

• #### $\phi$ $v_{3}/e_{3}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t100

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...

• #### $\Lambda$ $v_{3}/e_{3}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t101

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...

• #### $\Xi$ $v_{3}/e_{3}$($p_{\text{T}}$), Centrality 0-10%

10.17182/hepdata.102643.v1/t102

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...

• #### $K^{0}_{s}$ $v_{3}/e_{3}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t103

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...

• #### $\phi$ $v_{3}/e_{3}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t104

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...

• #### $\Lambda$ $v_{3}/e_{3}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t105

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...

• #### $\Xi$ $v_{3}/e_{3}$($p_{\text{T}}$), Centrality 10-40%

10.17182/hepdata.102643.v1/t106

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...

• #### $K^{0}_{s}$ $v_{3}/e_{3}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t107

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...

• #### $\phi$ $v_{3}/e_{3}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t108

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...

• #### $\Lambda$ $v_{3}/e_{3}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t109

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...

• #### $\Xi$ $v_{3}/e_{3}$($p_{\text{T}}$), Centrality 40-80%

10.17182/hepdata.102643.v1/t110

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...

• #### $K^{0}_{s}$ $v_{2}/(e_{2}n_{q})$($KE_{T}/n_{q}$), Cent. 0-10%

10.17182/hepdata.102643.v1/t111

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $\Lambda$ $v_{2}/(e_{2}n_{q})$($KE_{T}/n_{q}$), Cent. 0-10%

10.17182/hepdata.102643.v1/t112

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $\Xi$ $v_{2}/(e_{2}n_{q})$($KE_{T}/n_{q}$), Cent. 0-10%

10.17182/hepdata.102643.v1/t113

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $K^{0}_{s}$ $v_{2}/(e_{2}n_{q})$($KE_{T}/n_{q}$), Cent. 10-40%

10.17182/hepdata.102643.v1/t114

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $\Lambda$ $v_{2}/(e_{2}n_{q})$($KE_{T}/n_{q}$), Cent. 10-40%

10.17182/hepdata.102643.v1/t115

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $\Xi$ $v_{2}/(e_{2}n_{q})$($KE_{T}/n_{q}$), Cent. 10-40%

10.17182/hepdata.102643.v1/t116

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $K^{0}_{s}$ $v_{2}/(e_{2}n_{q})$($KE_{T}/n_{q}$), Cent. 40-80%

10.17182/hepdata.102643.v1/t117

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $\Lambda$ $v_{2}/(e_{2}n_{q})$($KE_{T}/n_{q}$), Cent. 40-80%

10.17182/hepdata.102643.v1/t118

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $\Xi$ $v_{2}/(e_{2}n_{q})$($KE_{T}/n_{q}$), Cent. 40-80%

10.17182/hepdata.102643.v1/t119

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $K^{0}_{s}$ $v_{3}/(e_{3}n_{q})$($KE_{T}/n_{q}$), Cent. 0-10%

10.17182/hepdata.102643.v1/t120

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $\Lambda$ $v_{3}/(e_{3}n_{q})$($KE_{T}/n_{q}$), Cent. 0-10%

10.17182/hepdata.102643.v1/t121

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $\Xi$ $v_{3}/(e_{3}n_{q})$($KE_{T}/n_{q}$), Cent. 0-10%

10.17182/hepdata.102643.v1/t122

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $K^{0}_{s}$ $v_{3}/(e_{3}n_{q})$($KE_{T}/n_{q}$), Cent. 10-40%

10.17182/hepdata.102643.v1/t123

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $\Lambda$ $v_{3}/(e_{3}n_{q})$($KE_{T}/n_{q}$), Cent. 10-40%

10.17182/hepdata.102643.v1/t124

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $\Xi$ $v_{3}/(e_{3}n_{q})$($KE_{T}/n_{q}$), Cent. 10-40%

10.17182/hepdata.102643.v1/t125

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $K^{0}_{s}$ $v_{3}/(e_{3}n_{q})$($KE_{T}/n_{q}$), Cent. 40-80%

10.17182/hepdata.102643.v1/t126

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $\Lambda$ $v_{3}/(e_{3}n_{q})$($KE_{T}/n_{q}$), Cent. 40-80%

10.17182/hepdata.102643.v1/t127

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $\Xi$ $v_{3}/(e_{3}n_{q})$($KE_{T}/n_{q}$), Cent. 40-80%

10.17182/hepdata.102643.v1/t128

$v_{n}$ coefficients, scaled by the number of constituent quarks $(n_{q})$ to the power $n/2$ and participant eccentricity $\varepsilon_{n}$, of identified...

• #### $K^{0}_{s}$ $v_{3}/v_{2}^{3/2}$($p_{T}$), Cent. 0-80%

10.17182/hepdata.102643.v1/t129

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

• #### $\phi$ $v_{3}/v_{2}^{3/2}$($p_{T}$), Cent. 0-80%

10.17182/hepdata.102643.v1/t130

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

• #### $\Lambda$ $v_{3}/v_{2}^{3/2}$($p_{T}$), Cent. 0-80%

10.17182/hepdata.102643.v1/t131

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

• #### $\Xi$ $v_{3}/v_{2}^{3/2}$($p_{T}$), Cent. 0-80%

10.17182/hepdata.102643.v1/t132

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

• #### $\Omega$ $v_{3}/v_{2}^{3/2}$($p_{T}$), Cent. 0-80%

10.17182/hepdata.102643.v1/t133

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

• #### $K^{0}_{s}$ $v_{4}/v_{2}^{2}$($p_{T}$), Cent. 0-80%

10.17182/hepdata.102643.v1/t134

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

• #### $\phi$ $v_{4}/v_{2}^{2}$($p_{T}$), Cent. 0-80%

10.17182/hepdata.102643.v1/t135

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

• #### $\Lambda$ $v_{4}/v_{2}^{2}$($p_{T}$), Cent. 0-80%

10.17182/hepdata.102643.v1/t136

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

• #### $\Xi$ $v_{4}/v_{2}^{2}$($p_{T}$), Cent. 0-80%

10.17182/hepdata.102643.v1/t137

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