The final wave function is written:
Following Menshikov [149], most authors use an analytical approximation of with its asymptotic form valid in the limit of infinite separation, since the main contribution to the matrix element integral comes from the region where the separation is large. The asymptotic wave function is characterized by a normalization constant C [149,150]. Recently Kino et al. [114] obtained a new value of C using Kamimura's variational wave function (Section 2.1.4, page ), calculated with the Gaussian basis functions in the Jacobi co-ordinate. As we have discussed, Kamimura's wave function treats the break up channel into directly, hence it gives an accurate description of asymptotic behaviour, while overcoming the difficulty of the Gaussian basis (``fast dumping'') by using a sufficiently large number of basis functions. The formation rates are proportional to the square of the constant C, and its new value decreased the predicted formation rates by 14% compared to an earlier calculation in Ref. [149] using the Adiabatic Representation, but increased them by 33% compared to Ref. [150] using a variational wave function with the Slater-type basis functions [110]. It is interesting to note that the Slater-type basis method, which was used so successfully in the energy level calculations (see Table 2.1), gives a less accurate description (assuming Kino et al. are correct) of the asymptotic wave function compared even to the Adiabatic Representation method, perhaps illustrating the difficulty in achieving a unified description of the non-adiabatic three body problem. In our analysis, the new value of C by Kino et al. is used.