The three transitions appear to be affected in a similar manner, consistent with the similar shapes of the corresponding Dyson orbitals. The location of the () minimum consistently shifts to lower eKE as D increases, and the width of the minimum becomes narrower. At the same time, the depth of the minimum increases as D changes from zero to ~0.4 a.u., but this trend reverses for larger values of D. For D  0.4 a.u., the entire () curve for each of the transitions gradually shifts upward with increasing D. This parametric trend accelerates as D approaches the critical value for binding an ℓ = 0 electron in the point-dipole field, Dc = 0.6393 a.u. (1.625 Debye). Our current implementation only allows for D values below the critical dipole (i.e. in the absence of dipole bound states). However, the rapid anisotropy change just below Dc signals significant changes in the outgoing electron wave function as its s component approaches the binding limit in the pointdipole field. To emphasize the rapid evolution of the () trends as D  Dc, all graphs in Fig. include the curves calculated with D = 0.6390 a.u. (i.e., just below Dc). In each case, the difference between the 0.6390 and 0.6 a.u. curves is more significant than that between 0.6 and 0.4 a.u.