Recently, the doubly differential cross section for double ionization of he
lium by fast bare carbon ions has been measured as a function of the longit
udinal momentum components of both electrons (see Bapat et al 2000). These
data show that the two electrons are preferentially emitted back to back. I
n this work we investigate the influence of various forms for the initial a
nd final state wavefunctions on the calculated doubly differential cross se
ctions in the first Born approximation. It is found that both an appropriat
e representation of the derivative discontinuities of the initial bound sta
te wavefunction at the two-particle coalescence points and of the Coulomb r
epulsion of the electrons in the final continuum state are necessary to rep
roduce this experimental feature. The accuracy of the calculated initial he
lium atom binding energy is not a reliable criterion for an adequate descri
ption of correlation effects in a collisional situation.