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

The STAR 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...

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