“…where Φ (0) (r, t) is the slow-varying zero-order adiabatic approximation for Φ(r, t), and Φ (1) (r, t) is the 'rapid' part of Φ(r, t), representing the so-called 'rescattering' correction to Φ (0) (r, t) [32,43]. To separate the 'slow' and 'rapid' parts of Φ(r, t), we deform the integration path in (9) to the contours utilized for the Green's function in equation ( 14). Moreover, for that part of contour integral, whose major contribution is given by the vicinity of t ′ = t, we expand the exponent of Green's function up to the term (t − t ′ ) 3 .…”