Mean square of p_{T} | |||
<p^2_{T}> [(GeV/c)^2] | +/-(stat.) | +/-(syst.) | |
p+p | 3.45 | 0.85 | 1.22 |
d+Au | 3.70 | 0.33 | 0.44 |
Nuclear absorption cross section | ||||
σ_abs [mb] | +(stat.) | -(stat.) | +(syst.) | -(syst.) |
0.0 | 3.8 | 0.0 | 2.1 | 0.0 |
Nuclear modicifation factor vs. p_{T} | |||||||
p_{T} [GeV/c] | R_dAu [1] | +/-(stat.) | +(syst.) | -(syst.) | (p+p stat.) | (p+p syst.) | (N_coll) |
0.63 | 1.10 | 0.26 | 0.37 | 0.31 | 0.04 | 0.13 | 0.17 |
1.45 | 1.27 | 0.26 | 0.39 | 0.35 | 0.04 | 0.13 | 0.17 |
2.40 | 0.66 | 0.35 | 0.27 | 0.17 | 0.15 | 0.09 | 0.17 |
Nuclear modicifation factor vs. centrality | |||||||||||||
<N_part> | N_part err | <N_coll> | N_coll err | b [fm] | b err | p_{T} [GeV/c] | R_dAu [1] | +/-(stat.) | +(syst.) | -(syst.) | (p+p stat.) | (p+p syst.) | (N_coll) |
5.7 | 0.7 | 4.8 | 0.6 | 6.7 | 0.8 | 0-3 | 1.06 | 0.27 | 0.39 | 0.30 | 0.04 | 0.14 | 0.12 |
13.3 | 2.3 | 12.7 | 2.3 | 4.1 | 0.8 | 0-3 | 1.15 | 0.21 | 0.41 | 0.33 | 0.04 | 0.14 | 0.12 |
Invariant cross section in p+p | ||||
p_{T} [GeV/c] | Bd^2σ/2πdydpT [nb/(GeV/c)^-2] | +/-(stat.) | +(syst.) | -(syst.) |
0.66 | 3.1 | 1.3 | 1.9 | 1.9 |
2.90 | 0.24 | 0.13 | 0.14 | 0.14 |
Invariant yield in d+Au | |||||
p_{T} [GeV/c] | Bd^2N/2πdydpT [(GeV/c)^-2] | +/-(stat.) | +(syst.) | -(syst.) | scale |
0.63 | 7.87 | 1.80 | 2.17 | 2.64 | 10^-7 |
1.45 | 4.69 | 0.96 | 1.29 | 1.43 | 10^-7 |
2.40 | 0.62 | 0.33 | 0.16 | 0.25 | 10^-7 |