“…by (2.18). As already pointed out in papers [23,54,57,[63][64][65][66], the coefficients n(1, σ, n) in the expansion (2.19)(hence also the one in the expansion (2.20)) is nothing but the DDM basis for the BCJ numerator of YM amplitude. While in the expansion (2.8), i.e., A = σ∈S n−3 C(σ)A L (n − 1, n, σ, 1), suppose we can rewrite the (n − 3)!…”