“…In this work, as in Refs. [19,35], the struck parton is assumed to possess a momentum q = (q + , q − , q ⊥ ) ∼ (λ 2 Q, Q, λQ), where Q is a hard scale and λ is a small dimensionless number. In the previous papers, the gluons off which the jet scatters were assumed to have a momentum k ∼ (λ 2 , λ 2 , λ)Q.…”