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Observation of an Energy-Dependent Difference in Elliptic Flow between Particles and Antiparticles in Relativistic Heavy Ion Collisions

The STAR collaboration
Phys.Rev.Lett. 110 (2013) 142301, 2013.

Abstract
Elliptic flow ($v_{2}$) values for identified particles at mid-rapidity in Au+Au collisions, measured by the STAR experiment in the Beam Energy Scan at RHIC at $\sqrt{s_{NN}}=$ 7.7--62.4 GeV, are presented. A beam-energy dependent difference of the values of $v_{2}$ between particles and corresponding anti-particles was observed. The difference increases with decreasing beam energy and is larger for baryons compared to mesons. This implies that, at lower energies, particles and anti-particles are not consistent with the universal number-of-constituent-quark (NCQ) scaling of $v_{2}$ that was observed at $\sqrt{s_{NN}}=$ 200 GeV.

  • Table 1

    Figure 1a

    10.17182/hepdata.102939.v1/t1

    The elliptic flow $v_{2}$ of protons and anti-protons as a function of the transverse momentum, $p_{T}$, for 0–80$\%$ central Au+Au...

  • Table 2

    Figure 1b

    10.17182/hepdata.102939.v1/t2

    The elliptic flow $v_{2}$ of protons and anti-protons as a function of the transverse momentum, $p_{T}$, for 0–80$\%$ central Au+Au...

  • Table 3

    Figure 1c

    10.17182/hepdata.102939.v1/t3

    The elliptic flow $v_{2}$ of protons and anti-protons as a function of the transverse momentum, $p_{T}$, for 0–80$\%$ central Au+Au...

  • Table 4

    Figure 1d

    10.17182/hepdata.102939.v1/t4

    The elliptic flow $v_{2}$ of protons and anti-protons as a function of the transverse momentum, $p_{T}$, for 0–80$\%$ central Au+Au...

  • Table 5

    Figure 1a bottom

    10.17182/hepdata.102939.v1/t5

    The elliptic flow $v_{2}$ of protons and anti-protons as a function of the transverse momentum, $p_{T}$, for 0–80$\%$ central Au+Au...

  • Table 6

    Figure 1b bottom

    10.17182/hepdata.102939.v1/t6

    The elliptic flow $v_{2}$ of protons and anti-protons as a function of the transverse momentum, $p_{T}$, for 0–80$\%$ central Au+Au...

  • Table 7

    Figure 1c bottom

    10.17182/hepdata.102939.v1/t7

    The elliptic flow $v_{2}$ of protons and anti-protons as a function of the transverse momentum, $p_{T}$, for 0–80$\%$ central Au+Au...

  • Table 8

    Figure 1d bottom

    10.17182/hepdata.102939.v1/t8

    The elliptic flow $v_{2}$ of protons and anti-protons as a function of the transverse momentum, $p_{T}$, for 0–80$\%$ central Au+Au...

  • Table 9

    Figure 2

    10.17182/hepdata.102939.v1/t9

    The difference in $v_{2}$ between particles $(X)$ and their corresponding anti-particles $(X)$ (see legend) as a function of $\sqrt(s_{NN})$ for...

  • Table 10

    Figure 3a

    10.17182/hepdata.102939.v1/t10

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 11

    Figure 3a

    10.17182/hepdata.102939.v1/t11

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 12

    Figure 3a

    10.17182/hepdata.102939.v1/t12

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 13

    Figure 3a

    10.17182/hepdata.102939.v1/t13

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 14

    Figure 3a

    10.17182/hepdata.102939.v1/t14

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 15

    Figure 3a

    10.17182/hepdata.102939.v1/t15

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 16

    Figure 3a

    10.17182/hepdata.102939.v1/t16

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 17

    Figure 3b

    10.17182/hepdata.102939.v1/t17

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 18

    Figure 3b

    10.17182/hepdata.102939.v1/t18

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 19

    Figure 3b

    10.17182/hepdata.102939.v1/t19

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 20

    Figure 3b

    10.17182/hepdata.102939.v1/t20

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 21

    Figure 3b

    10.17182/hepdata.102939.v1/t21

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 22

    Figure 3b

    10.17182/hepdata.102939.v1/t22

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 23

    Figure 3b

    10.17182/hepdata.102939.v1/t23

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 24

    Figure 3b

    10.17182/hepdata.102939.v1/t24

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 25

    Figure 3c

    10.17182/hepdata.102939.v1/t25

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 26

    Figure 3c

    10.17182/hepdata.102939.v1/t26

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 27

    Figure 3c

    10.17182/hepdata.102939.v1/t27

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 28

    Figure 3c

    10.17182/hepdata.102939.v1/t28

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 29

    Figure 3c

    10.17182/hepdata.102939.v1/t29

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 30

    Figure 3c

    10.17182/hepdata.102939.v1/t30

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 31

    Figure 3c

    10.17182/hepdata.102939.v1/t31

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 32

    Figure 3d

    10.17182/hepdata.102939.v1/t32

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 33

    Figure 3d

    10.17182/hepdata.102939.v1/t33

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 34

    Figure 3d

    10.17182/hepdata.102939.v1/t34

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 35

    Figure 3d

    10.17182/hepdata.102939.v1/t35

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 36

    Figure 3d

    10.17182/hepdata.102939.v1/t36

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 37

    Figure 3d

    10.17182/hepdata.102939.v1/t37

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 38

    Figure 3d

    10.17182/hepdata.102939.v1/t38

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 39

    Figure 3d

    10.17182/hepdata.102939.v1/t39

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 40

    Figure 3a bottom

    10.17182/hepdata.102939.v1/t40

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 41

    Figure 3a bottom

    10.17182/hepdata.102939.v1/t41

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 42

    Figure 3a bottom

    10.17182/hepdata.102939.v1/t42

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 43

    Figure 3b bottom

    10.17182/hepdata.102939.v1/t43

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 44

    Figure 3b bottom

    10.17182/hepdata.102939.v1/t44

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 45

    Figure 3b bottom

    10.17182/hepdata.102939.v1/t45

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 46

    Figure 3b bottom

    10.17182/hepdata.102939.v1/t46

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 47

    Figure 3c bottom

    10.17182/hepdata.102939.v1/t47

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 48

    Figure 3c bottom

    10.17182/hepdata.102939.v1/t48

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 49

    Figure 3c bottom

    10.17182/hepdata.102939.v1/t49

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 50

    Figure 3d bottom

    10.17182/hepdata.102939.v1/t50

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 51

    Figure 3d bottom

    10.17182/hepdata.102939.v1/t51

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 52

    Figure 3d bottom

    10.17182/hepdata.102939.v1/t52

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 53

    Figure 3d bottom

    10.17182/hepdata.102939.v1/t53

    The upper panels depict the elliptic flow, $v_{2}$, as a function of reduced transverse mass, $(m_{T} − m_{0})$, for particles,...

  • Table 54

    Figure 4a

    10.17182/hepdata.102939.v1/t54

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 55

    Figure 4a

    10.17182/hepdata.102939.v1/t55

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 56

    Figure 4a

    10.17182/hepdata.102939.v1/t56

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 57

    Figure 4a

    10.17182/hepdata.102939.v1/t57

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 58

    Figure 4a

    10.17182/hepdata.102939.v1/t58

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 59

    Figure 4a

    10.17182/hepdata.102939.v1/t59

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 60

    Figure 4a

    10.17182/hepdata.102939.v1/t60

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 61

    Figure 4b

    10.17182/hepdata.102939.v1/t61

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 62

    Figure 4b

    10.17182/hepdata.102939.v1/t62

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 63

    Figure 4b

    10.17182/hepdata.102939.v1/t63

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 64

    Figure 4b

    10.17182/hepdata.102939.v1/t64

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 65

    Figure 4b

    10.17182/hepdata.102939.v1/t65

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 66

    Figure 4b

    10.17182/hepdata.102939.v1/t66

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 67

    Figure 4b

    10.17182/hepdata.102939.v1/t67

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 68

    Figure 4b

    10.17182/hepdata.102939.v1/t68

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 69

    Figure 4c

    10.17182/hepdata.102939.v1/t69

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 70

    Figure 4c

    10.17182/hepdata.102939.v1/t70

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 71

    Figure 4c

    10.17182/hepdata.102939.v1/t71

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 72

    Figure 4c

    10.17182/hepdata.102939.v1/t72

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 73

    Figure 4d

    10.17182/hepdata.102939.v1/t73

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 74

    Figure 4d

    10.17182/hepdata.102939.v1/t74

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 75

    Figure 4d

    10.17182/hepdata.102939.v1/t75

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 76

    Figure 4d

    10.17182/hepdata.102939.v1/t76

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 77

    Figure 4a bottom

    10.17182/hepdata.102939.v1/t77

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 78

    Figure 4a bottom

    10.17182/hepdata.102939.v1/t78

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 79

    Figure 4a bottom

    10.17182/hepdata.102939.v1/t79

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 80

    Figure 4a bottom

    10.17182/hepdata.102939.v1/t80

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 81

    Figure 4a bottom

    10.17182/hepdata.102939.v1/t81

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 82

    Figure 4a bottom

    10.17182/hepdata.102939.v1/t82

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 83

    Figure 4a bottom

    10.17182/hepdata.102939.v1/t83

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 84

    Figure 4b bottom

    10.17182/hepdata.102939.v1/t84

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 85

    Figure 4b bottom

    10.17182/hepdata.102939.v1/t85

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 86

    Figure 4b bottom

    10.17182/hepdata.102939.v1/t86

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 87

    Figure 4b bottom

    10.17182/hepdata.102939.v1/t87

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 88

    Figure 4b bottom

    10.17182/hepdata.102939.v1/t88

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 89

    Figure 4b bottom

    10.17182/hepdata.102939.v1/t89

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 90

    Figure 4b bottom

    10.17182/hepdata.102939.v1/t90

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 91

    Figure 4b bottom

    10.17182/hepdata.102939.v1/t91

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 92

    Figure 4c bottom

    10.17182/hepdata.102939.v1/t92

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 93

    Figure 4c bottom

    10.17182/hepdata.102939.v1/t93

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 94

    Figure 4c bottom

    10.17182/hepdata.102939.v1/t94

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 95

    Figure 4c bottom

    10.17182/hepdata.102939.v1/t95

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 96

    Figure 4d bottom

    10.17182/hepdata.102939.v1/t96

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 97

    Figure 4d bottom

    10.17182/hepdata.102939.v1/t97

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 98

    Figure 4d bottom

    10.17182/hepdata.102939.v1/t98

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

  • Table 99

    Figure 4c bottom

    10.17182/hepdata.102939.v1/t99

    The number-of-constituent quark scaled elliptic flow $(v_{2}/n_{q})((m_{T} − m_{0})/n_{q})$ for 0–80$\%$ central Au+Au collisions at $\sqrt{s_{NN}}$ = 11.5 and 62.4...

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