We consider normalized Slater-type orbitals nlm(α)(q) in the momentum space representation. The following general Fourier transform of these functions is obtained:
where Cnλ and Ylm represents the usual Gegenbauer polynomials and spherical harmonics, respectively. This unified analytical formula is valid for all the allowed values of integer n – l. Previous results, which are given in terms of the Gauss hypergeometric function 2F1, provide two separate expressions depending upon whether n – l is odd or even. A power series representation of the present result for nlm(α)(q) contains the vector q merely through regular solid harmonics ql Ylm () and binomial terms (q2 + α2)−N, where N is a non-negative integer. This is particularly amenable to subsequent integrations over the vector q in multicenter atomic scattering integrals involving the momentum space Slater-type orbitals.