Centrality dependence of charged and strange hadron elliptic flow from 200 GeV Au+Au collisions
B.I. Abelev et al, arXiv:0801.3466, submitted to Phys. Rev. C.
Figure 1: invariant mass distribution and v2 vs. minv for Kshort, Lambda, Cascade and Omega, centrality 0 - 80%, from Au+Au collisions at sqrt(sNN) = 200 GeV.
png | eps
invarant mass data
Figure 3: v2(eta) for charged hadrons, 0.15 < pT < 2.0 GeV/c, centrality 10 - 40%, from Au+Au collisions at sqrt(sNN) = 200 GeV.
png | eps
eta | v2{LYZ} (%) |
v2{EP} (%) |
-4.05 | 2.12 | +/- 0.708 | 2.41 | +/- 0.214 |
-3.95 | 2.59 | +/- 0.377 | 2.12 | +/- 0.103 |
-3.85 | 3.01 | +/- 0.242 | 2.51 | +/- 0.0703 |
-3.75 | 2.83 | +/- 0.207 | 2.64 | +/- 0.0589 |
-3.65 | 3.05 | +/- 0.193 | 2.7 | +/- 0.0542 |
-3.55 | 2.84 | +/- 0.182 | 2.82 | +/- 0.0517 |
-3.45 | 2.94 | +/- 0.16 | 2.87 | +/- 0.0501 |
-3.35 | 2.96 | +/- 0.175 | 2.94 | +/- 0.0492 |
-3.25 | 3.05 | +/- 0.173 | 2.97 | +/- 0.0489 |
-3.15 | 3.07 | +/- 0.175 | 3.18 | +/- 0.0487 |
-3.05 | 3.04 | +/- 0.175 | 3.03 | +/- 0.049 |
-2.95 | 2.97 | +/- 0.17 | 3.02 | +/- 0.0503 |
-2.85 | 3.06 | +/- 0.174 | 2.99 | +/- 0.0546 |
-2.75 | 3.04 | +/- 0.233 | 2.91 | +/- 0.0679 |
-2.65 | 3.18 | +/- 0.425 | 2.8 | +/- 0.111 |
-1.05 | 4.88 | +/- 0.112 | 5.58 | +/- 0.0315 |
-0.95 | 4.98 | +/- 0.0952 | 5.58 | +/- 0.0272 |
-0.85 | 4.96 | +/- 0.0919 | 5.62 | +/- 0.0259 |
-0.75 | 5.09 | +/- 0.0803 | 5.72 | +/- 0.0255 |
-0.65 | 5.05 | +/- 0.085 | 5.71 | +/- 0.0254 |
-0.55 | 4.93 | +/- 0.0928 | 5.67 | +/- 0.0254 |
-0.45 | 5.12 | +/- 0.0847 | 5.82 | +/- 0.0254 |
-0.35 | 4.98 | +/- 0.0845 | 5.8 | +/- 0.0255 |
-0.25 | 4.95 | +/- 0.084 | 5.8 | +/- 0.0255 |
-0.15 | 5.02 | +/- 0.0891 | 5.84 | +/- 0.0256 |
-0.05 | 4.98 | +/- 0.0883 | 5.81 | +/- 0.0256 |
0.05 | 5.15 | +/- 0.0786 | 5.81 | +/- 0.0256 |
0.15 | 5.08 | +/- 0.0813 | 5.79 | +/- 0.0256 |
0.25 | 5 | +/- 0.0863 | 5.8 | +/- 0.0254 |
0.35 | 4.97 | +/- 0.0807 | 5.81 | +/- 0.0254 |
0.45 | 5.03 | +/- 0.0841 | 5.85 | +/- 0.0253 |
0.55 | 5 | +/- 0.0852 | 5.74 | +/- 0.0253 |
0.65 | 4.86 | +/- 0.0899 | 5.71 | +/- 0.0253 |
0.75 | 5.14 | +/- 0.0868 | 5.68 | +/- 0.0254 |
0.85 | 4.99 | +/- 0.0875 | 5.68 | +/- 0.0258 |
0.95 | 4.9 | +/- 0.0939 | 5.56 | +/- 0.027 |
1.05 | 4.94 | +/- 0.0989 | 5.66 | +/- 0.0312 |
2.65 | 3.05 | +/- 0.342 | 2.94 | +/- 0.0907 |
2.75 | 3.13 | +/- 0.196 | 3.07 | +/- 0.0585 |
2.85 | 3.02 | +/- 0.171 | 3.04 | +/- 0.0493 |
2.95 | 3.03 | +/- 0.147 | 3.13 | +/- 0.0471 |
3.05 | 3.11 | +/- 0.143 | 3.12 | +/- 0.0466 |
3.15 | 3.21 | +/- 0.162 | 3.07 | +/- 0.0469 |
3.25 | 3.05 | +/- 0.149 | 2.99 | +/- 0.0473 |
3.35 | 3.07 | +/- 0.164 | 3.07 | +/- 0.0477 |
3.45 | 3.05 | +/- 0.163 | 3.01 | +/- 0.0488 |
3.55 | 2.94 | +/- 0.164 | 2.89 | +/- 0.0506 |
3.65 | 2.73 | +/- 0.173 | 2.87 | +/- 0.0532 |
3.75 | 2.4 | +/- 0.184 | 2.64 | +/- 0.0578 |
3.85 | 2.55 | +/- 0.236 | 2.5 | +/- 0.0677 |
3.95 | 2.58 | +/- 0.298 | 2.34 | +/- 0.0953 |
4.05 | 1.85 | +/- 0.609 | 2.29 | +/- 0.19 |
PHOBOS
Figure 4: v2(pT) for charged hadrons, centrality 10 - 40%, from Au+Au collisions at sqrt(sNN) = 200 GeV.
png | eps
pT | 10-40% v2{EP} (%) |
0.259284 | 2.41931 | +/- 0.00362892 |
0.444508 | 4.43858 | +/- 0.00365882 |
0.64248 | 6.49861 | +/- 0.00448379 |
0.842139 | 8.35248 | +/- 0.00566996 |
1.04207 | 10.0155 | +/- 0.00720866 |
1.242 | 11.5316 | +/- 0.00918359 |
1.44191 | 12.9486 | +/- 0.0117265 |
1.64184 | 14.2383 | +/- 0.0150116 |
1.8622 | 15.4317 | +/- 0.0177037 |
2.19969 | 16.8996 | +/- 0.019479 |
2.70153 | 18.1805 | +/- 0.035862 |
3.20461 | 18.3824 | +/- 0.0639516 |
3.708 | 17.7214 | +/- 0.109534 |
4.35898 | 16.8977 | +/- 0.150454 |
5.38528 | 14.8173 | +/- 0.338867 |
6.66575 | 13.4716 | +/- 0.560351 |
pT | 10-40% v2{4} (%) |
0.330488 | 3.0627 | +/- 0.00767071 |
0.552691 | 5.28566 | +/- 0.00955173 |
0.777641 | 7.25672 | +/- 0.0126261 |
1.00265 | 8.99126 | +/- 0.0167758 |
1.22784 | 10.4889 | +/- 0.0222966 |
1.4529 | 11.8553 | +/- 0.0295949 |
1.67785 | 12.979 | +/- 0.0394646 |
1.90279 | 13.9013 | +/- 0.052586 |
2.12772 | 14.7467 | +/- 0.0699616 |
2.3528 | 15.2095 | +/- 0.0932843 |
2.578 | 15.5902 | +/- 0.123354 |
2.80337 | 15.6635 | +/- 0.161997 |
3.02893 | 15.2927 | +/- 0.212332 |
3.33996 | 15.4851 | +/- 0.214673 |
3.79249 | 14.5577 | +/- 0.342653 |
4.24483 | 13.6088 | +/- 0.53047 |
4.69808 | 12.7122 | +/- 0.785808 |
5.15102 | 9.92637 | +/- 1.13733 |
5.60383 | 11.1757 | +/- 1.53568 |
6.05393 | 11.1025 | +/- 2.02217 |
pT | 10-40% v2{LYZ} |
0.1 | 0.0145518 | +/- 0.000497656 |
0.3 | 0.0252366 | +/- 0.000231103 |
0.5 | 0.0445516 | +/- 0.000272429 |
0.7 | 0.0617433 | +/- 0.000354682 |
0.9 | 0.0771507 | +/- 0.000526592 |
1.1 | 0.091119 | +/- 0.000618766 |
1.3 | 0.103573 | +/- 0.000799947 |
1.5 | 0.114753 | +/- 0.00104875 |
1.7 | 0.124094 | +/- 0.00136385 |
1.9 | 0.133199 | +/- 0.00167784 |
2.1 | 0.146204 | +/- 0.00229006 |
2.3 | 0.150116 | +/- 0.00284306 |
2.5 | 0.156712 | +/- 0.00361734 |
2.7 | 0.153915 | +/- 0.00451628 |
3 | 0.161012 | +/- 0.00475137 |
3.4 | 0.161405 | +/- 0.00712341 |
3.8 | 0.146103 | +/- 0.0106279 |
4.2 | 0.146748 | +/- 0.0161081 |
4.7 | 0.117731 | +/- 0.0195912 |
5.5 | 0.104679 | +/- 0.0277295 |
pT | 0-80% v2{EP} (%) |
0.25 | 2.28 | +/- 0.011 |
0.35 | 3.21 | +/- 0.011 |
0.45 | 4.14 | +/- 0.012 |
0.55 | 5.1 | +/- 0.014 |
0.65 | 5.95 | +/- 0.015 |
0.75 | 6.78 | +/- 0.017 |
0.85 | 7.58 | +/- 0.02 |
0.95 | 8.33 | +/- 0.022 |
1.05 | 9.02 | +/- 0.025 |
1.15 | 9.66 | +/- 0.029 |
1.25 | 10.3 | +/- 0.032 |
1.35 | 11 | +/- 0.036 |
1.45 | 11.5 | +/- 0.041 |
1.55 | 12.1 | +/- 0.047 |
1.65 | 12.8 | +/- 0.053 |
1.75 | 13.3 | +/- 0.06 |
1.85 | 13.8 | +/- 0.068 |
1.95 | 14.1 | +/- 0.077 |
2.05 | 14.6 | +/- 0.088 |
2.15 | 14.9 | +/- 0.1 |
2.25 | 15.4 | +/- 0.11 |
2.35 | 15.8 | +/- 0.13 |
2.45 | 15.8 | +/- 0.14 |
2.55 | 16.1 | +/- 0.16 |
2.65 | 16.6 | +/- 0.19 |
2.75 | 16.8 | +/- 0.21 |
2.85 | 17.1 | +/- 0.24 |
2.95 | 17.5 | +/- 0.27 |
3.05 | 17.4 | +/- 0.3 |
3.15 | 17.1 | +/- 0.33 |
3.25 | 17.3 | +/- 0.38 |
3.35 | 16.8 | +/- 0.42 |
3.45 | 17.6 | +/- 0.47 |
3.55 | 16.7 | +/- 0.53 |
3.65 | 15.6 | +/- 0.58 |
3.75 | 17.3 | +/- 0.65 |
3.85 | 17.3 | +/- 0.72 |
3.95 | 17.7 | +/- 0.79 |
4.25 | 17 | +/- 0.47 |
4.75 | 16.8 | +/- 0.7 |
5.25 | 14.4 | +/- 1 |
5.75 | 14 | +/- 1.3 |
Figure 5: v2 for charged hadrons, from Au+Au collisions at sqrt(sNN) = 200 GeV.
png | eps
Collision Cross Section | v2{EP}(%) |
70-80% | 6.96 | +/- 0.089 |
60-70% | 7.23 | +/- 0.049 |
50-60% | 7.44 | +/- 0.028 |
40-50% | 7.4 | +/- 0.019 |
30-40% | 7.03 | +/- 0.014 |
20-30% | 6.18 | +/- 0.011 |
10-20% | 4.76 | +/- 0.01 |
5-10% | 3.39 | +/- 0.014 |
0-5% | 2.32 | +/- 0.017 |
Collision Cross Section | v2{4}(%) |
60-70% | 5.81859 | +/- 0.0947424 |
50-60% | 6.17547 | +/- 0.0318834 |
40-50% | 6.55523 | +/- 0.0144613 |
30-40% | 6.30763 | +/- 0.00873136 |
20-30% | 5.63609 | +/- 0.00674778 |
10-20% | 4.25772 | +/- 0.00805643 |
5-10% | 2.69707 | +/- 0.0241449 |
Collision Cross Section | v2{LYZ_Sum} |
40-50% | 0.0581909 | +/- 0.00115924 |
30-40% | 0.059935 | +/- 0.000298429 |
20-30% | 0.0541134 | +/- 0.000171784 |
10-20% | 0.0411426 | +/- 0.0002367 |
Collision Cross Section | v2{LYZ_Prod}(%) |
50-60% | 6.3 | +/- 0.37 |
40-50% | 6.27 | +/- 0.17 |
30-40% | 6.12 | +/- 0.03 |
20-30% | 5.41 | +/- 0.024 |
10-20% | 4.04 | +/- 0.032 |
5-10% | 2.92 | +/- 0.23 |
Figure 6: v2 as a function of pT for K short and Lambda from different flow methods, from 10-40% Au+Au collisions at sqrt(sNN) = 200 GeV.
png | eps
pT | Lambda v2{EtaSub} |
0.514949 | 0.0171887 | +/- 0.00599847 |
0.711084 | 0.0252045 | +/- 0.00259926 |
0.904933 | 0.0439538 | +/- 0.00166433 |
1.10191 | 0.0669239 | +/- 0.00142684 |
1.29762 | 0.0892634 | +/- 0.00136037 |
1.49586 | 0.112365 | +/- 0.00138535 |
1.69476 | 0.132239 | +/- 0.00150687 |
1.89409 | 0.147663 | +/- 0.00172608 |
2.09326 | 0.172195 | +/- 0.00203265 |
2.29311 | 0.183985 | +/- 0.0024701 |
2.49256 | 0.191453 | +/- 0.00306674 |
2.69237 | 0.204347 | +/- 0.00381858 |
2.96933 | 0.216477 | +/- 0.00380066 |
3.36913 | 0.229389 | +/- 0.00619977 |
3.77169 | 0.21872 | +/- 0.00819382 |
4.17067 | 0.233404 | +/- 0.0127392 |
4.64291 | 0.188215 | +/- 0.0181105 |
pT | Kshort v2{EtaSub} |
0.317096 | 0.0100251 | +/- 0.00408946 |
0.509452 | 0.0320396 | +/- 0.00168157 |
0.702165 | 0.0561704 | +/- 0.00111416 |
0.898215 | 0.0768067 | +/- 0.000970017 |
1.09519 | 0.0996481 | +/- 0.00103237 |
1.29427 | 0.113964 | +/- 0.00117545 |
1.49361 | 0.128467 | +/- 0.00141058 |
1.69317 | 0.140205 | +/- 0.00176012 |
1.89283 | 0.14309 | +/- 0.00219019 |
2.09255 | 0.154878 | +/- 0.00274344 |
2.29251 | 0.168122 | +/- 0.00347806 |
2.49212 | 0.163106 | +/- 0.0044512 |
2.69255 | 0.162033 | +/- 0.00564722 |
2.97062 | 0.171903 | +/- 0.00559919 |
3.37197 | 0.181144 | +/- 0.00838975 |
3.7753 | 0.142844 | +/- 0.0115172 |
4.17461 | 0.137889 | +/- 0.0169962 |
4.64733 | 0.103468 | +/- 0.0196233 |
pT | Lambda v2{EP} |
0.514949 | 0.0094109 | +/- 0.00323675 |
0.711084 | 0.0224248 | +/- 0.00139298 |
0.904933 | 0.0394955 | +/- 0.000874296 |
1.10191 | 0.0597768 | +/- 0.000753618 |
1.29762 | 0.0832616 | +/- 0.000730031 |
1.49586 | 0.105047 | +/- 0.000759209 |
1.69476 | 0.126631 | +/- 0.000832138 |
1.89409 | 0.143083 | +/- 0.000952359 |
2.09326 | 0.162732 | +/- 0.00112346 |
2.29311 | 0.174088 | +/- 0.00136522 |
2.49256 | 0.187091 | +/- 0.00168906 |
2.69237 | 0.195022 | +/- 0.00210206 |
2.96933 | 0.21034 | +/- 0.00208083 |
3.36913 | 0.215933 | +/- 0.00338213 |
3.77169 | 0.218885 | +/- 0.00446477 |
4.17067 | 0.214503 | +/- 0.00705484 |
4.64291 | 0.20487 | +/- 0.00970422 |
pT | Kshort v2{EP} |
0.317096 | 0.0079846 | +/- 0.00209356 |
0.509452 | 0.0302893 | +/- 0.000896153 |
0.702165 | 0.0520612 | +/- 0.000603296 |
0.898215 | 0.0734969 | +/- 0.000517407 |
1.09519 | 0.094635 | +/- 0.000546628 |
1.29427 | 0.110096 | +/- 0.00062781 |
1.49361 | 0.12326 | +/- 0.000766214 |
1.69317 | 0.134534 | +/- 0.000964707 |
1.89283 | 0.141625 | +/- 0.00120641 |
2.09255 | 0.148651 | +/- 0.00151602 |
2.29251 | 0.154482 | +/- 0.00192347 |
2.49212 | 0.157332 | +/- 0.0024439 |
2.69255 | 0.160623 | +/- 0.00309508 |
2.97062 | 0.161147 | +/- 0.00302011 |
3.37197 | 0.164409 | +/- 0.0045633 |
3.7753 | 0.149344 | +/- 0.00632754 |
4.17461 | 0.156241 | +/- 0.00898313 |
pT | Lambda v2{LYZ} |
0.7 | 0.0204249 | +/- 0.0161687 |
0.9 | 0.0449429 | +/- 0.0103231 |
1.1 | 0.0576095 | +/- 0.00848428 |
1.3 | 0.0742113 | +/- 0.00857593 |
1.5 | 0.095503 | +/- 0.00828999 |
1.7 | 0.117663 | +/- 0.00918476 |
1.9 | 0.130515 | +/- 0.0102733 |
2.1 | 0.145503 | +/- 0.0116361 |
2.3 | 0.153935 | +/- 0.0142901 |
2.5 | 0.168661 | +/- 0.0180623 |
2.7 | 0.191726 | +/- 0.0215367 |
3 | 0.191704 | +/- 0.0225114 |
3.4 | 0.195716 | +/- 0.0332879 |
3.8 | 0.214813 | +/- 0.0448018 |
4.2 | 0.21607 | +/- 0.0645706 |
4.7 | 0.167517 | +/- 0.0840312 |
pT | Kshort v2{LYZ} |
0.7 | 0.046447 | +/- 0.00656214 |
0.9 | 0.0663339 | +/- 0.00575719 |
1.1 | 0.0896825 | +/- 0.00616352 |
1.3 | 0.0990288 | +/- 0.00703264 |
1.5 | 0.10631 | +/- 0.00830646 |
1.7 | 0.11786 | +/- 0.0103924 |
1.9 | 0.134167 | +/- 0.012838 |
2.1 | 0.147435 | +/- 0.016086 |
2.3 | 0.143746 | +/- 0.0192996 |
2.5 | 0.149837 | +/- 0.024233 |
2.7 | 0.115113 | +/- 0.0306358 |
3 | 0.127617 | +/- 0.0295145 |
3.4 | 0.152779 | +/- 0.0415067 |
3.8 | 0.170774 | +/- 0.0540181 |
4.2 | 0.145372 | +/- 0.0695473 |
4.7 | 0.0329796 | +/- 0.0809972 |
Figure 7: v2 as a function of pT for different centralities, from Au+Au collisions at sqrt(sNN) = 200 GeV.
png | eps
pT | Kshort 0-80% v2{EP} | Kshort 40-80% v2{EP} | Kshort 10-40% v2{EP} | Kshort 0-10% v2{EP} |
0.317 | 0.0082 | +/- 0.0018 | +/- 0.0005 | 0.0192 | +/- 0.0034 | +/- 0.0011 | 0.0080 | +/- 0.0021 | +/- 0.0005 | -0.0053 | +/- 0.0051 | +/- 0.0004 |
0.509 | 0.0286 | +/- 0.0007 | +/- 0.0016 | 0.0465 | +/- 0.0016 | +/- 0.0027 | 0.0302 | +/- 0.0008 | +/- 0.0017 | 0.0070 | +/- 0.0020 | +/- 0.0005 |
0.701 | 0.0480 | +/- 0.0005 | +/- 0.0015 | 0.0748 | +/- 0.0012 | +/- 0.0024 | 0.0520 | +/- 0.0006 | +/- 0.0017 | 0.0191 | +/- 0.0012 | +/- 0.0011 |
0.898 | 0.0665 | +/- 0.0004 | +/- 0.0022 | 0.1037 | +/- 0.0010 | +/- 0.0034 | 0.0734 | +/- 0.0005 | +/- 0.0024 | 0.0295 | +/- 0.0010 | +/- 0.0012 |
1.094 | 0.0849 | +/- 0.0004 | +/- 0.0028 | 0.1258 | +/- 0.0011 | +/- 0.0041 | 0.0946 | +/- 0.0005 | +/- 0.0031 | 0.0416 | +/- 0.0010 | +/- 0.0018 |
1.294 | 0.0988 | +/- 0.0005 | +/- 0.0032 | 0.1470 | +/- 0.0013 | +/- 0.0048 | 0.1100 | +/- 0.0006 | +/- 0.0036 | 0.0499 | +/- 0.0011 | +/- 0.0021 |
1.493 | 0.1106 | +/- 0.0006 | +/- 0.0036 | 0.1617 | +/- 0.0017 | +/- 0.0053 | 0.1232 | +/- 0.0007 | +/- 0.0040 | 0.0581 | +/- 0.0014 | +/- 0.0025 |
1.692 | 0.1213 | +/- 0.0008 | +/- 0.0040 | 0.1778 | +/- 0.0021 | +/- 0.0058 | 0.1345 | +/- 0.0009 | +/- 0.0044 | 0.0631 | +/- 0.0017 | +/- 0.0027 |
1.892 | 0.1288 | +/- 0.0010 | +/- 0.0042 | 0.1816 | +/- 0.0027 | +/- 0.0060 | 0.1416 | +/- 0.0012 | +/- 0.0046 | 0.0739 | +/- 0.0021 | +/- 0.0031 |
2.092 | 0.1342 | +/- 0.0012 | +/- 0.0044 | 0.1877 | +/- 0.0034 | +/- 0.0062 | 0.1486 | +/- 0.0015 | +/- 0.0049 | 0.0745 | +/- 0.0027 | +/- 0.0032 |
2.292 | 0.1391 | +/- 0.0016 | +/- 0.0046 | 0.1947 | +/- 0.0043 | +/- 0.0064 | 0.1544 | +/- 0.0019 | +/- 0.0051 | 0.0756 | +/- 0.0035 | +/- 0.0032 |
2.492 | 0.1443 | +/- 0.0020 | +/- 0.0047 | 0.2076 | +/- 0.0054 | +/- 0.0068 | 0.1573 | +/- 0.0024 | +/- 0.0052 | 0.0778 | +/- 0.0045 | +/- 0.0033 |
2.692 | 0.1464 | +/- 0.0026 | +/- 0.0048 | 0.2087 | +/- 0.0068 | +/- 0.0069 | 0.1606 | +/- 0.0030 | +/- 0.0053 | 0.0763 | +/- 0.0058 | +/- 0.0033 |
2.969 | 0.1484 | +/- 0.0025 | +/- 0.0049 | 0.2117 | +/- 0.0064 | +/- 0.0070 | 0.1611 | +/- 0.0030 | +/- 0.0053 | 0.0777 | +/- 0.0056 | +/- 0.0033 |
3.371 | 0.1495 | +/- 0.0038 | +/- 0.0049 | 0.196 | +/- 0.0097 | +/- 0.0065 | 0.1644 | +/- 0.0045 | +/- 0.0054 | 0.0824 | +/- 0.0086 | +/- 0.0036 |
3.774 | 0.1423 | +/- 0.0053 | +/- 0.0109 | 0.2025 | +/- 0.0124 | +/- 0.0155 | 0.1493 | +/- 0.0063 | +/- 0.0088 | 0.0715 | +/- 0.0133 | +/- 0.0183 |
4.175 | 0.1436 | +/- 0.0077 | +/- 0.0110 | 0.2089 | +/- 0.0173 | +/- 0.0160 | 0.1562 | +/- 0.0089 | +/- 0.0120 | 0.0591 | +/- 0.0189 | +/- 0.0153 |
4.648 | 0.1348 | +/- 0.0092 | +/- 0.0280 | 0.2257 | +/- 0.0216 | +/- 0.0261 | 0.1204 | +/- 0.0108 | +/- 0.0193 | 0.0849 | +/- 0.0212 | +/- 0.0218 |
5.38 | 0.1274 | +/- 0.0124 | +/- 0.0265 | 0.1932 | +/- 0.0288 | +/- 0.0223 | 0.1287 | +/- 0.0146 | +/- 0.0207 | 0.0666 | +/- 0.0297 | +/- 0.0171 |
6.393 | 0.1031 | +/- 0.0261 | +/- 0.0214 | | | | 0.0949 | +/- 0.0312 | +/- 0.0152 | | | |
pT | Lambda 0-80% v2{EP} | Lambda 40-80% v2{EP} | Lambda 10-40% v2{EP} | Lambda 0-10% v2{EP} |
0.515 | 0.0099 | +/- 0.0027 | +/- 0.0005 | 0.0333 | +/- 0.0052 | +/- 0.0021 | 0.0094 | +/- 0.0032 | +/- 0.0007 | -0.0123 | +/- 0.0075 | +/- 0.0009 |
0.710 | 0.0219 | +/- 0.0011 | +/- 0.0007 | 0.0494 | +/- 0.0026 | +/- 0.0016 | 0.0224 | +/- 0.0013 | +/- 0.0007 | -0.0049 | +/- 0.0028 | +/- 0.0002 |
0.904 | 0.0379 | +/- 0.0007 | +/- 0.0012 | 0.0726 | +/- 0.0017 | +/- 0.0024 | 0.0394 | +/- 0.00086 | +/- 0.0013 | 0.0083 | +/- 0.0017 | +/- 0.0003 |
1.101 | 0.0566 | +/- 0.0006 | +/- 0.0018 | 0.1007 | +/- 0.0015 | +/- 0.0033 | 0.0597 | +/- 0.0007 | +/- 0.0019 | 0.0217 | +/- 0.0014 | +/- 0.0009 |
1.297 | 0.0766 | +/- 0.0006 | +/- 0.0025 | 0.1319 | +/- 0.0016 | +/- 0.0043 | 0.0832 | +/- 0.0007 | +/- 0.0027 | 0.0321 | +/- 0.0013 | +/- 0.0014 |
1.495 | 0.0942 | +/- 0.0006 | +/- 0.0031 | 0.1559 | +/- 0.0017 | +/- 0.0051 | 0.1050 | +/- 0.0007 | +/- 0.0034 | 0.0423 | +/- 0.0013 | +/- 0.0018 |
1.694 | 0.1115 | +/- 0.0007 | +/- 0.0036 | 0.1795 | +/- 0.0019 | +/- 0.0059 | 0.1266 | +/- 0.0008 | +/- 0.0041 | 0.0522 | +/- 0.0014 | +/- 0.0022 |
1.893 | 0.1271 | +/- 0.0008 | +/- 0.0042 | 0.2053 | +/- 0.0023 | +/- 0.0068 | 0.1430 | +/- 0.0009 | +/- 0.0047 | 0.0644 | +/- 0.0016 | +/- 0.0028 |
2.093 | 0.1419 | +/- 0.0009 | +/- 0.0047 | 0.2179 | +/- 0.0027 | +/- 0.0072 | 0.1627 | +/- 0.0011 | +/- 0.0053 | 0.0732 | +/- 0.0019 | +/- 0.0031 |
2.292 | 0.1525 | +/- 0.0011 | +/- 0.0050 | 0.2325 | +/- 0.0034 | +/- 0.0077 | 0.1740 | +/- 0.0013 | +/- 0.0057 | 0.0819 | +/- 0.0023 | +/- 0.0035 |
2.492 | 0.1648 | +/- 0.0014 | +/- 0.0054 | 0.2519 | +/- 0.0042 | +/- 0.0083 | 0.1870 | +/- 0.0016 | +/- 0.0062 | 0.0904 | +/- 0.0028 | +/- 0.0039 |
2.692 | 0.1725 | +/- 0.0017 | +/- 0.0057 | 0.261 | +/- 0.0053 | +/- 0.0086 | 0.1950 | +/- 0.0021 | +/- 0.0064 | 0.0971 | +/- 0.0036 | +/- 0.0042 |
2.969 | 0.1831 | +/- 0.0017 | +/- 0.0060 | 0.2667 | +/- 0.0052 | +/- 0.0088 | 0.2103 | +/- 0.0020 | +/- 0.0069 | 0.0995 | +/- 0.0036 | +/- 0.0043 |
3.368 | 0.1912 | +/- 0.0028 | +/- 0.0063 | 0.2821 | +/- 0.0083 | +/- 0.0093 | 0.2159 | +/- 0.0033 | +/- 0.0071 | 0.1081 | +/- 0.0058 | +/- 0.0047 |
3.770 | 0.2001 | +/- 0.0039 | +/- 0.0153 | 0.2818 | +/- 0.0097 | +/- 0.0216 | 0.2188 | +/- 0.0044 | +/- 0.0143 | 0.1175 | +/- 0.0091 | +/- 0.0136 |
4.170 | 0.1968 | +/- 0.0060 | +/- 0.0151 | 0.2816 | +/- 0.0146 | +/- 0.0216 | 0.2145 | +/- 0.0070 | +/- 0.0140 | 0.1108 | +/- 0.0140 | +/- 0.0128 |
4.639 | 0.1924 | +/- 0.0083 | +/- 0.0222 | 0.2677 | +/- 0.0198 | +/- 0.0205 | 0.2048 | +/- 0.0097 | +/- 0.0134 | 0.1165 | +/- 0.0203 | +/- 0.0242 |
5.357 | 0.2023 | +/- 0.0144 | +/- 0.0325 | 0.2863 | +/- 0.0318 | +/- 0.0331 | 0.2210 | +/- 0.0162 | +/- 0.0255 | 0.0941 | +/- 0.0370 | +/- 0.0196 |
pT | Cascade 0-80% v2{EP} |
0.722563 | 0.0261114 | +/- 0.0139645 |
1.00463 | 0.0392122 | +/- 0.00717688 |
1.20326 | 0.0475371 | +/- 0.00515703 |
1.40283 | 0.0689692 | +/- 0.00439337 |
1.60118 | 0.0915935 | +/- 0.00401599 |
1.79935 | 0.103817 | +/- 0.00395525 |
1.9976 | 0.119726 | +/- 0.00402313 |
2.19736 | 0.143823 | +/- 0.00441006 |
2.44004 | 0.158223 | +/- 0.0041712 |
2.73913 | 0.166251 | +/- 0.00527452 |
3.26503 | 0.182095 | +/- 0.00505404 |
4.42511 | 0.190342 | +/- 0.0160431 |
pT | Cascade 40-80% v2{EP} |
0.869569 | 0.0752325 | +/- 0.0138365 |
1.20339 | 0.0863737 | +/- 0.0126111 |
1.40199 | 0.112248 | +/- 0.0109697 |
1.60092 | 0.137503 | +/- 0.0107076 |
1.79946 | 0.15517 | +/- 0.0109892 |
2.08409 | 0.182669 | +/- 0.00866405 |
2.54915 | 0.23 | +/- 0.00993906 |
3.19048 | 0.282273 | +/- 0.0162859 |
4.12584 | 0.311723 | +/- 0.034606 |
pT | Cascade 10-40% v2{EP} |
0.842228 | 0.0320598 | +/- 0.00980172 |
1.31536 | 0.0608806 | +/- 0.00491283 |
1.70072 | 0.11075 | +/- 0.0041424 |
2.08848 | 0.145376 | +/- 0.00438282 |
2.55586 | 0.177799 | +/- 0.00483978 |
3.19791 | 0.187871 | +/- 0.00782921 |
4.09988 | 0.237557 | +/- 0.0168438 |
pT | Cascade 0-10% v2{EP} |
0.843151 | -0.00306532 | +/- 0.00969649 |
1.31722 | 0.0253973 | +/- 0.00412047 |
1.7942 | 0.0498181 | +/- 0.00273099 |
2.32384 | 0.0838206 | +/- 0.00333611 |
2.88204 | 0.097858 | +/- 0.00430378 |
3.6897 | 0.101919 | +/- 0.00786869 |
4.89013 | 0.104234 | +/- 0.0273729 |
pT | Omega 0-80% v2{EP} |
1.32915 | 0.0661981 | +/- 0.0241724 |
2.05904 | 0.0999717 | +/- 0.0132867 |
2.72859 | 0.137056 | +/- 0.0193252 |
3.30277 | 0.187048 | +/- 0.022867 |
4.12384 | 0.171189 | +/- 0.0456596 |
pT | Omega 0-10% v2{EP} |
1.31269 | 0.0121919 | +/- 0.0368811 |
2.06737 | 0.0487778 | +/- 0.0161611 |
2.73245 | 0.0649741 | +/- 0.0215874 |
3.21721 | 0.0808476 | +/- 0.0295293 |
3.85145 | 0.0866268 | +/- 0.0336264 |
pT | Proton 0-80% v2 |
2.7 | 0.180246 | +/- 0.00290963 |
2.9 | 0.181065 | +/- 0.00345699 |
3.1 | 0.178428 | +/- 0.000595242 |
3.37869 | 0.181223 | +/- 7.49683e-05 |
3.78035 | 0.189231 | +/- 0.0118001 |
4.1822 | 0.181522 | +/- 0.0103588 |
4.58477 | 0.188166 | +/- 0.0182788 |
5.1134 | 0.154632 | +/- 0.02227 |
5.7 | 0.196634 | +/- 0.0394095 |
6.4 | 0.170919 | +/- 0.0565542 |
pT | Pion 0-80% v2 |
2.7 | 0.150636 | +/- 0.0017354 |
2.9 | 0.152232 | +/- 0.0024031 |
3.1 | 0.144395 | +/- 5.16337e-05 |
3.37869 | 0.142593 | +/- 4.15058e-05 |
3.78035 | 0.134701 | +/- 0.00453809 |
4.1822 | 0.130562 | +/- 0.00631406 |
4.58477 | 0.132124 | +/- 0.00928315 |
5.1134 | 0.105676 | +/- 0.00904789 |
5.7 | 0.112569 | +/- 0.0168643 |
6.4 | 0.0988393 | +/- 0.0203937 |
Figure 8: v2 as a function of mT-m for different centralities, from Au+Au collisions at sqrt(sNN) = 200 GeV.
png | eps
v2 in Fig. 7 is re-plotted as a function of mT-m.
Figure 9: v2/nq vs. pT/nq and v2/nq vs. (mT-m)/nq for 0-80% from Au+Au collisions at sqrt(sNN) = 200 GeV.
png | eps
v2 in Fig. 7(a) divided by nq vs. pT/nq
and vs. (mT-m)/nq.
Data/Fit are shown.
phi data
Figure 10,11: v2/nq vs. pT/nq and v2/nq vs. (mT-m)/nq for 0-10%, 10-40% and 40-80% from Au+Au collisions at sqrt(sNN) = 200 GeV.
fig10 png | fig10 eps
fig11 png | fig11 eps
v2 in Fig. 7(b), (c) and (d) divided by nq vs. pT/nq
and vs. (mT-m)/nq
Data/Fit are shown.
Figure 12: scaling properties for 0-10%, 10-40% and 40-80% from Au+Au collisions at sqrt(sNN) = 200 GeV.
png | eps
Fig. 12 (a) and (b): v2 in Fig. 10 scaled by participant eccentricity in Tab. I for the corresponding centrality bin.
Fig. 12 (c): v2 in Fig. 10 scaled by pT-integrated v2 of each particle in Tab. II.
Fig. 12 (d): v2 in Fig. 10 scaled by pT-integrated v2 of charged particle.
Collision Cross Section | charged particle pT-integrated v2 |
0-10% | 0.0283 | +/- 0.000112 |
10-40% | 0.0576 | +/- 0.000064 |
40-80% | 0.0735 | +/- 0.000163 |
Fig. 12 (d) inset: expansion at low pT.
pT | Kshort v2 |
0.25 | -0.00829987 | +/- 0.0124875 |
0.35 | -0.0063051 | +/- 0.00618741 |
0.45 | 0.00511618 | +/- 0.00349805 |
0.55 | 0.00833931 | +/- 0.00240646 |
0.65 | 0.0148362 | +/- 0.00187736 |
0.75 | 0.0226785 | +/- 0.00156796 |
0.85 | 0.0274998 | +/- 0.00144415 |
0.95 | 0.0319449 | +/- 0.00142249 |
pT | Lambda v2 |
0.45 | -0.0124351 | +/- 0.0184532 |
0.55 | -0.0116623 | +/- 0.00796461 |
0.65 | -0.00686117 | +/- 0.00484526 |
0.75 | -0.00361544 | +/- 0.00355683 |
0.85 | 0.00636274 | +/- 0.00267256 |
0.95 | 0.0100045 | +/- 0.00233125 |
Figure 13: centrality dependence of participant eccentricity scaled v2 versus number of participants from Au+Au collisions at sqrt(sNN) = 200 GeV.
png | eps
Identified particle value: v2 in Tab. II scaled by participant eccentricity in Tab. I versus number of participant in Tab. I.
Charged particle
Npart | &epsilonpart | v2 |
14.05 | 0.6683 | 0.0696 | +/- 0.00089 |
26.93 | 0.5712 | 0.0723 | +/- 0.00049 |
47.25 | 0.4935 | 0.0744 | +/- 0.00028 |
76.66 | 0.4269 | 0.0740 | +/- 0.00019 |
115.49 | 0.3597 | 0.0703 | +/- 0.00014 |
166.63 | 0.2873 | 0.0618 | +/- 0.00011 |
234.54 | 0.2019 | 0.0476 | +/- 0.00010 |
298.87 | 0.130 | 0.0339 | +/- 0.00014 |
351.90 | 0.0854 | 0.0232 | +/- 0.00017 |
Figure 14: energy dependence of participant eccentricity scaled v2
png | eps
62.4 GeV data
17.2 GeV data
pT | Kshort v2 |
0.1752 | -0.026008 | +/- 0.0214718 |
0.5007 | 0.0108871 | +/- 0.0133065 |
0.8012 | 0.0078629 | +/- 0.013004 |
1.10172 | 0.0290323 | +/- 0.019354 |
1.40219 | 0.0508065 | +/- 0.0296371 |
1.72144 | 0.0840726 | +/- 0.0462702 |
2.1471 | 0.104032 | +/- 0.0967742 |
pT | Lambda v2 |
0.54545 | -0.0169355 | +/- 0.0157258 |
0.92163 | 0.0024193 | +/- 0.009375 |
1.17241 | 0.0072580 | +/- 0.0081653 |
1.4232 | 0.0314516 | +/- 0.00877016 |
1.67398 | 0.0514113 | +/- 0.0117944 |
1.92476 | 0.0592742 | +/- 0.0148185 |
2.17555 | 0.0774194 | +/- 0.0193548 |
2.42006 | 0.0737903 | +/- 0.0257056 |
2.79624 | 0.131855 | +/- 0.0266129 |
3.29154 | 0.138508 | +/- 0.0462702 |
Figure 15: energy dependence of participant eccentricity scaling properties
png | eps
62.4 GeV data
200 GeV data is the same as in Fig 12(b).
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