momentum particles in hadron-hadron collisions,” Phys. Rev. D 75 , 114014 (2007) [ arXiv:0705.2141 [hep-ph]]. 

[69] The uncertainties of the dense and sparse cross-hatched bands are partially correlated because they share the same contribution from Λ$_{QCD}$ and α$_{MS}$ . The correlated contributions should be removed when checking the consistency of the two bands. The agreement is still excellent when only the uncertainties from the α$_{V}$ series truncation at two loops for the sparse cross- hatched band and the uncertainties on the CSR series truncation for the dense cross-hatched band are used to estimate the band widths. 

[70] The cross-hatched band could be computed only for Q 2 > ∼ 3 GeV 2 because, as already noticed, the perturbative series in the MS scheme is less suitable for low Q 2 studies: the leading-order scale shift in the present case is Q ∗ = 0 . 368 Q . 

