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Table 8:

High-energy biases on the W03 cross-section set.

W03
$K_0^{\rm best}\times 10^2$ $\delta^{\rm best}$ $V_{\rm c}^{\rm best}$ $V_{\rm a}^{\rm best}$ $\chi^2$/d.o.f.
HE bias x (kpc2 Myr-1)   (km$\;$s-1) (km$\;$s-1)  
0: +0.05 4.05 0.45 ... ... 26.5
0: +0.02 4.06 0.42 ... ... 27.7
0:  ${\it +0.00}$ 4.08 0.40 ... ... 28.8
0: -0.02 4.09 0.38 ... ... 30.1
0: -0.05 4.13 0.34 ... ... 32.5

I: +0.05 0.61 0.89 13.7 ... 12.1
I: +0.02 0.49 0.91 13.6 ... 11.4
I:  ${\it +0.00}$ 0.42 0.93 13.5 ... 11.2
I: -0.02 0.35 0.95 13.4 ... 11.2
I: -0.05 0.27 0.98 13.1 ... 11.8

II: +0.05 9.20 0.28 ... 78.0 3.26
II: +0.02 9.51 0.25 ... 75.0 4.13
II:  ${\it +0.00}$ 9.76 0.23 ... 73.1 4.73
II: -0.02 10.0 0.21 ... 71.2 5.35
II: -0.05 10.4 0.19 ... 68.1 6.27

III: +0.05 0.98 0.74 19.0 50.0 1.01
III: +0.02 0.75 0.81 19.0 42.7 1.22
III:  ${\it +0.00}$ 0.48 0.86 18.8 38.0 1.47
III: -0.02 0.35 0.91 18.5 33.4 1.88
III: -0.05 0.21 1.01 17.8 26.6 2.94

Notes. Models 0, I, II, and III for L=4 kpc. The various sets are obtained after multiplying the W03 set by $(E_{\rm k/n})^{x}$above 1 GeV/n (and kept constant above 10 GeV/n), with x=+0.05, +0.02, 0, -0.02, -0.05. (corresponding to bottom to top curves on the right-hand side of Fig. 3).


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