“…By the smooth coefficients of (3.2)-(3.4), we have that the first order perturbations satisfy a linearized system and are well defined for (t, ξ) ∈ R + × R. Similar to the argument of [3,4], we express the quantities w, v, σ appearing in (2.7) in terms of (X, U, L, A, B, Q). More specifically, we see that (1) The shift in x is computed by…”