Centrality and pseudorapidity dependence of charged hadron production at intermediate pT in Au+Au collisions at sqrt(sNN) = 200 GeV
J. Adams et al Phys. Rev. C 70(2004) 044901.


Figure 3: Number of binary collisions and participants from different models.

Ratios are used in Fig.3. Here we give the numbers and errors of Npart and Nbin from different models instead.  
CentralityHIJINGVENUSMC Glauber
NpartNbinaryNpartNbinaryNpartNbinary
 (0-5)%353+/-13957+/-67346+/-14872+/-57352+3-41020+71-68
(5-10)%300+/-14749+/-61293+/-14694+/-50298+5-7804+64-63
(10-20)%233+/-15523+/-52228+/-15496+/-46234+8-8575+56-55
(20-30)%164+/-13318+/-41161+/-13311+/-37166+10-9359+46-44
(30-40)%112+/-12183+/-30111+/-11187+/-28115+11-9215+36-33
(40-60)%58+/-1075+/-1758+/-980+/-1761+10-791+23-19
(60-80)%18+/-616+/-620+/-619+/-721+6-521+7-8

Figure 4: Invariant differential yield, 0.5 < |η| < 1

Errors are combined statistical and systematic.                
(1/2πpT)d2N/dpTdη (0.5<|η|<1) [(GeV/c)-2]
pT[GeV/c]  (0-5)% (5-10)%  (10-20)%  (20-30)%  (30-40)%  (40-60)%  (60-80)%
0.25302+/-27250+/- 21173+/- 19118+/-9.775.8+/-6.138.6+/-3.112.1+/-0.97
0.35204+/-18160+/- 14116+/-1379.6+/-6.551.2+/-424.7+/-27.28+/-0.57
0.45130+/-11102+/-8.774.3+/-848.1+/-3.930.9+/-2.414.9+/-1.24.64+/-0.36
0.5583+/-7.365.2+/-5.647.5+/-5.130.7+/-2.519.7+/-1.59.5+/-0.762.8+/-0.22
0.6556+/-4.944+/-3.832+/-3.520.7+/-1.713.3+/-16.41+/-0.521.79+/-0.15
0.7537.8+/-3.328.1+/-2.420.5+/-2.214+/-1.18.5+/-0.654.09+/-0.331.14+/-0.089
0.8525.6+/-2.220.1+/-1.713.8+/-1.59.44+/-0.776.07+/-0.472.76+/-0.220.729+/-0.057
0.9517.3+/-1.513.5+/-1.29.32+/-  16.38+/-0.524.1+/-0.321.87+/-0.150.492+/-0.04
1.0511.6+/-  19.67+/-0.836.66+/-0.724.55+/-0.372.77+/-0.221.26+/-0.10.314+/-0.025
1.158.32+/-0.726.53+/-0.564.5+/-0.493.07+/-0.251.87+/-0.150.851+/-0.0690.224+/-0.018
1.255.62+/-0.494.66+/-0.43.21+/-0.352.2+/-0.181.33+/-0.110.608+/-0.0490.151+/-0.012
1.354.01+/-0.353.15+/-0.272.29+/-0.251.57+/-0.130.953+/-0.0750.434+/-0.0350.102+/-0.0079
1.452.86+/-0.252.25+/-0.191.64+/-0.181.06+/-0.0870.681+/-0.0540.293+/-0.0240.073+/-0.0058
1.552.05+/-0.181.61+/-0.141.17+/-0.130.756+/-0.0620.486+/-0.0390.221+/-0.0180.0493+/-0.0039
1.651.38+/-0.121.15+/-0.0980.835+/-0.090.54+/-0.0440.328+/-0.0260.149+/-0.0120.0373+/-0.003
1.751.04+/-0.0890.819+/-0.070.596+/-0.0640.386+/-0.0320.234+/-0.0190.107+/-0.00860.0266+/-0.0023
1.850.745+/-0.0640.585+/-0.050.426+/-0.0460.275+/-0.0230.177+/-0.0150.0806+/-0.00650.019+/-0.0016
1.950.532+/-0.0470.418+/-0.0360.304+/-0.0330.208+/-0.0170.126+/-0.0110.0575+/-0.00460.0144+/-0.0012
2.050.38+/-0.0330.298+/-0.0250.217+/-0.0230.157+/-0.0130.0903+/-0.00770.0411+/-0.00340.0102+/-0.00089
2.150.271+/-0.0240.213+/-0.0180.164+/-0.0180.106+/-0.00870.0645+/-0.00530.0294+/-0.00260.00774+/-0.00068
2.250.194+/-0.0170.161+/-0.0140.117+/-0.0130.0757+/-0.00620.0487+/-0.00410.0222+/-0.00190.00553+/-0.0005
2.350.138+/-0.0120.115+/-0.00980.0837+/-0.0090.0572+/-0.00470.0348+/-0.00310.0167+/-0.00150.00395+/-0.00037
2.450.0883+/-0.00810.0733+/-0.00630.0534+/-0.00590.0365+/-0.00320.0235+/-0.00190.0107+/-0.000920.00238+/-0.00021
2.690.0476+/-0.00570.0418+/-0.00470.0305+/-0.00410.0208+/-0.00210.0134+/-0.00130.0061+/-0.000550.00152+/-0.00015
2.890.0272+/-0.00310.0226+/-0.00250.0174+/-0.00230.0126+/-0.00120.00723+/-0.000710.00368+/-0.000350.000918+/-0.0001
3.160.0124+/-0.00150.0109+/-0.00130.00838+/-0.00110.00542+/-0.000530.00369+/-0.000360.00177+/-0.000170.000524+/-5.6e-05
3.550.00427+/-0.000520.00375+/-0.000440.00305+/-0.000410.00221+/-0.000230.00142+/-0.000150.000723+/-7.3e-05 0.00017+/-2.2e-05
4.060.00124+/-0.000160.00103+/-0.000130.000794+/-0.000140.000574+/-6.6e-050.000437+/-5e-050.000199+/-2.2e-054.19e-05+/-7.2e-06
4.700.000289+/-4.2e-050.000253+/-3.7e-050.000207+/-3.8e-050.000149+/-2.1e-050.000107+/-1.6e-056.48e-05+/-8.7e-061.71e-05+/-3.8e-06
5.485.67e-05+/-1e-054.98e-05+/-1.1e-054.8e-05+/-1.1e-052.94e-05+/-5.7e-062.23e-05+/-4.8e-068.12e-06+/-1.9e-065.56e-06+/-1.6e-06

Figures 5 and 6: Ratio of invariant differential yield, (0.5 < |η| < 1)/(|η|<0.5)

Errors are combined statistical and systematic.     
(d2N/dpTdη(0.5<|η|<1))/(d2N/dpTdη(|η|<0.5))
pT[GeV/c](0-5)%(5-10)%(10-20)%(20-30)%(30-40)%(40-60)%(60-80)%
0.250.96+/-0.070.96+/-0.070.96+/-0.070.96+/-0.070.97+/-0.070.96+/-0.070.97+/-0.07
0.350.96+/-0.070.96+/-0.070.96+/-0.070.97+/-0.070.98+/-0.070.97+/-0.070.97+/-0.07
0.450.96+/-0.070.96+/-0.070.97+/-0.070.97+/-0.070.99+/-0.070.97+/-0.070.97+/-0.07
0.550.96+/-0.070.96+/-0.070.96+/-0.070.97+/-0.070.97+/-0.070.96+/-0.070.97+/-0.07
0.650.95+/-0.070.95+/-0.070.96+/-0.070.97+/-0.070.98+/-0.070.97+/-0.070.95+/-0.07
0.750.95+/-0.070.95+/-0.070.95+/-0.070.97+/-0.070.97+/-0.070.97+/-0.070.96+/-0.07
0.850.95+/-0.070.95+/-0.070.96+/-0.070.97+/-0.070.97+/-0.070.97+/-0.070.97+/-0.07
0.950.95+/-0.070.96+/-0.070.96+/-0.070.96+/-0.070.98+/-0.070.97+/-0.070.94+/-0.07
1.050.95+/-0.070.95+/-0.070.95+/-0.070.97+/-0.070.98+/-0.070.97+/-0.070.95+/-0.07
1.150.95+/-0.070.95+/-0.070.94+/-0.070.97+/-0.070.97+/-0.070.96+/-0.070.97+/-0.07
1.25    0.95+/-0.070.95+/-0.070.96+/-0.070.97+/-0.070.98+/-0.070.96+/-0.070.93+/-0.07
1.35    0.95+/-0.070.95+/-0.070.96+/-0.070.96+/-0.070.98+/-0.070.97+/-0.070.93+/-0.07
1.45    0.95+/-0.070.94+/-0.070.95+/-0.070.96+/-0.070.97+/-0.070.96+/-0.070.96+/-0.07
1.55    0.95+/-0.070.94+/-0.070.94+/-0.070.95+/-0.070.96+/-0.070.97+/-0.070.90+/-0.07
1.65    0.95+/-0.070.94+/-0.070.94+/-0.070.94+/-0.070.95+/-0.070.97+/-0.070.93+/-0.07
1.75    0.95+/-0.070.94+/-0.070.94+/-0.070.95+/-0.070.96+/-0.070.96+/-0.070.91+/-0.07
1.85    0.94+/-0.070.94+/-0.070.94+/-0.070.94+/-0.070.94+/-0.070.96+/-0.070.97+/-0.08
1.95    0.94+/-0.070.94+/-0.070.95+/-0.070.95+/-0.070.93+/-0.071.00+/-0.070.97+/-0.09
2.05    0.94+/-0.070.95+/-0.070.95+/-0.070.96+/-0.070.94+/-0.070.93+/-0.070.91+/-0.08
2.15    0.94+/-0.080.94+/-0.080.95+/-0.080.91+/-0.080.90+/-0.070.92+/-0.070.98+/-0.09
2.25    0.95+/-0.080.93+/-0.080.95+/-0.090.92+/-0.080.95+/-0.080.94+/-0.080.94+/-0.09
2.35    0.93+/-0.090.94+/-0.090.93+/-0.090.98+/-0.090.91+/-0.090.98+/-0.090.94+/-0.10
2.45    0.94+/-0.090.94+/-0.100.94+/-0.090.94+/-0.090.95+/-0.090.91+/-0.080.85+/-0.09
2.69    0.94+/-0.100.95+/-0.100.94+/-0.100.87+/-0.090.96+/-0.100.95+/-0.090.96+/-0.11
2.89    0.93+/-0.100.93+/-0.100.95+/-0.100.94+/-0.100.89+/-0.090.96+/-0.100.90+/-0.11
3.16    0.93+/-0.100.93+/-0.100.93+/-0.110.89+/-0.100.94+/-0.100.90+/-0.091.04+/-0.13
3.55    0.92+/-0.110.93+/-0.110.97+/-0.120.96+/-0.111.04+/-0.130.99+/-0.110.95+/-0.15
4.06    0.91+/-0.120.87+/-0.110.89+/-0.120.89+/-0.121.10+/-0.160.88+/-0.120.59+/-0.12
4.70    0.92+/-0.150.89+/-0.140.83+/-0.150.79+/-0.141.00+/-0.201.06+/-0.191.02+/-0.31
5.48    0.96+/-0.200.93+/-0.191.06+/-0.270.79+/-0.211.04+/-0.320.64+/-0.201.38+/-0.61

Figure 7: dN/dη distributions for pT > 2 GeV/c and |η|<1, scaled by Nbin and divided by NN reference.

Errors are combined statistical and systematic errors for data and do not include errors from NN reference.         
(1/Nbin)dN/dη(pT>2)/(dN/dη(pT>2)(NN))
η(0-5)%(5-10)%(10-20)%(30-40)%(40-60)%(60-80)%
 -0.950.60+/-0.090.61+/-0.090.67+/-0.090.75+/-0.110.78+/-0.110.85+/-0.13
 -0.850.61+/-0.090.63+/-0.090.68+/-0.090.76+/-0.110.79+/-0.110.85+/-0.13
 -0.750.63+/-0.090.65+/-0.090.68+/-0.090.78+/-0.110.82+/-0.110.86+/-0.13
 -0.650.64+/-0.090.67+/-0.090.70+/-0.100.76+/-0.110.86+/-0.120.96+/-0.14
 -0.550.65+/-0.090.67+/-0.090.70+/-0.100.79+/-0.110.87+/-0.120.96+/-0.14
 -0.450.65+/-0.090.68+/-0.100.71+/-0.100.79+/-0.110.89+/-0.130.90+/-0.13
 -0.350.67+/-0.090.70+/-0.100.73+/-0.100.84+/-0.120.88+/-0.120.98+/-0.14
 -0.250.67+/-0.090.70+/-0.100.72+/-0.100.82+/-0.120.88+/-0.121.00+/-0.15
 -0.150.65+/-0.090.69+/-0.100.72+/-0.100.83+/-0.120.86+/-0.120.96+/-0.14
 -0.050.64+/-0.090.67+/-0.090.72+/-0.100.83+/-0.120.89+/-0.131.01+/-0.15
0.050.64+/-0.090.68+/-0.090.71+/-0.100.80+/-0.110.86+/-0.120.91+/-0.13
0.150.64+/-0.090.67+/-0.090.72+/-0.100.79+/-0.110.87+/-0.120.97+/-0.14
0.250.65+/-0.090.69+/-0.100.71+/-0.100.82+/-0.110.88+/-0.130.91+/-0.13
0.350.64+/-0.090.69+/-0.100.70+/-0.100.80+/-0.110.86+/-0.121.02+/-0.15
0.450.64+/-0.090.65+/-0.090.71+/-0.100.75+/-0.110.84+/-0.120.97+/-0.14
0.550.62+/-0.090.65+/-0.090.70+/-0.100.75+/-0.110.82+/-0.110.92+/-0.13
0.650.61+/-0.090.63+/-0.090.67+/-0.090.75+/-0.110.81+/-0.120.92+/-0.14
0.750.61+/-0.090.64+/-0.090.68+/-0.100.76+/-0.100.79+/-0.110.91+/-0.13
0.850.59+/-0.080.63+/-0.090.65+/-0.090.75+/-0.100.83+/-0.120.92+/-0.14
0.950.57+/-0.080.62+/-0.090.63+/-0.090.73+/-0.100.83+/-0.120.77+/-0.12

Figure 8a: Ratio of charged hadron yields within |η|<1 for Au+Au relative to the NN reference, scaled by Npart/2 and divided by NN reference, for a pT bin at 2.05 GeV/c.

Errors are combined statistical and systematic errors for data and do not include errors from NN reference.
Npart (2/Npart)(d2N/dpTdη(|η|<1,AA))/(d2N/dpTdη(|η|<1,NN)))), pT = 2.05 GeV/c
211.82+/- 0.18
612.43+/- 0.24
1152.84+/- 0.29
1663.26+/- 0.33
2343.45+/- 0.37
2983.68+/- 0.39
3523.84+/- 0.39

Figure 8b: Participant scaling exponent ν of charged hardron yields as a function of pT within |η|<1.

Errors are combined statistical and systematic errors for data and do not include errors from NN reference.
 pT [GeV/c]  ν(|η|<1)
0.25 1.131+/-0.036
0.35 1.147+/-0.036
0.45 1.172+/-0.033
0.55 1.189+/-0.033
0.65 1.208+/-0.036
0.75 1.217+/-0.033
0.85 1.236+/-0.036
0.95 1.247+/-0.036
1.05 1.256+/-0.033
1.15 1.264+/-0.036
1.25 1.275+/-0.036
1.35 1.278+/-0.039
1.45 1.283+/-0.039
1.55 1.283+/-0.039
1.65 1.283+/-0.039
1.75 1.281+/-0.042
1.85 1.286+/-0.042
1.95 1.278+/-0.039
2.05 1.269+/-0.042
2.15 1.261+/-0.044
2.25 1.256+/-0.044
2.35 1.244+/-0.044
2.45 1.244+/-0.061
2.69 1.225+/-0.058
2.89 1.194+/-0.056
3.16 1.156+/-0.056
3.55 1.147+/-0.058
4.06 1.103+/-0.058
4.70 1.008+/-0.069
5.48 0.942+/-0.097

Figure 9: Ratio of truncated mean pT for pT>pTcut within |η|<1 in Au+Au collisions to that in NN reference as a function of pTcut.

Errors are combined statistical and systematic errors for data and do not include errors from NN reference.
<pTtrunc>(pT>pTcut, |η|<1,AA)/<pTtrunc>(pT>pTcut, |η|<1,NN)
pTcut [GeV/c]      (0-5)%       (60-80)%
0.20 1.283+/-0.0271.155+/-0.025
0.30 1.260+/-0.0271.147+/-0.023
0.40 1.238+/-0.0251.143+/-0.023
0.50 1.215+/-0.0251.138+/-0.025
0.60 1.192+/-0.0251.133+/-0.023
0.70 1.167+/-0.0271.127+/-0.023
0.80 1.142+/-0.0251.123+/-0.023
0.90 1.117+/-0.0231.115+/-0.025
1.00 1.092+/-0.0251.108+/-0.025
1.10 1.067+/-0.0231.102+/-0.025
1.20 1.043+/-0.0231.095+/-0.025
1.30 1.020+/-0.0231.082+/-0.025
1.40 1.002+/-0.0251.077+/-0.023
1.50 0.983+/-0.0231.068+/-0.025
1.60 0.967+/-0.0231.058+/-0.025
1.70 0.950+/-0.0231.055+/-0.025
1.80 0.937+/-0.0231.052+/-0.025
1.90 0.922+/-0.0221.040+/-0.027
2.00 0.913+/-0.0231.033+/-0.027
2.10 0.908+/-0.0251.034+/-0.028
2.20 0.898+/-0.0251.034+/-0.029
2.30 0.893+/-0.0271.033+/-0.031
2.40 0.883+/-0.0271.027+/-0.033
2.60 0.870+/-0.0271.012+/-0.035
2.80 0.857+/-0.0300.990+/-0.040
3.00 0.853+/-0.0330.987+/-0.047
3.35 0.848+/-0.0381.035+/-0.062
3.80 0.837+/-0.0431.060+/-0.087

Figure 10: Binary scaling fraction in pT>pTcut within |η|<1 as a function of centrality.

Errors include combined statistical and systematic errors and those propagated from Npart and Nbin/Npart.

Binary scaling fraction=F(|η|<1)
pTcut[GeV/c]
Npart0.21.02.03.8
210.065+/-0.5220.620+/-0.3700.908+/-0.2990.957+/-0.337
610.239+/-0.2070.728+/-0.1300.897+/-0.1030.875+/-0.147
1150.326+/-0.1300.761+/-0.0760.891+/-0.0650.799+/-0.114
1660.391+/-0.0980.788+/-0.0600.897+/-0.0490.788+/-0.103
2340.435+/-0.0760.799+/-0.0490.880+/-0.0430.755+/-0.092
2980.478+/-0.0650.810+/-0.0380.875+/-0.0380.707+/-0.098
3520.527+/-0.0600.821+/-0.0380.875+/-0.0380.679+/-0.103

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