“…The scaling of the relevant degrees of freedom, in light-cone coordinates (p + , p − , p ⊥ ), can be written in terms of λ as collinear: p µ c ∼ Q(λ 2 , 1, λ) n soft: p µ s ∼ Q(λ, λ, λ) n . (2.13) Q is the typical hard scale and n µ = (1, 0, 0, 1) is the four-vector along which we expand in light-cone coordinates, 14) where p − = n • p, p + =n • p, andn µ = (1, 0, 0, −1) such that n 2 =n 2 = 0 and n •n = 2. We separate the label and residual components of momenta as follows:…”