We discuss the properties of a simple and robust scheme for preparing atoms
and molecules in an arbitrary preselected coherent superposition of quantu
m states-fractional stimulated Raman adiabatic passage (fractional STIRAP)-
first proposed by Marte el al (1991 Phys. Rev. A 44 R4118). As in STIRAP, t
he Stokes pulse arrives before the pump purse, but unlike STIRAP, here the
two pulses terminate simultaneously, while maintaining a constant ratio of
amplitudes. We extend earlier research and suggest a realization of this sc
heme with two smoothly varying delayed laser pulses (which can be derived f
rom a single laser), the parameters of the created superposition being cont
rolled by the polarization of the delayed pulse. Furthermore, we provide si
mple analytic estimates of the robustness of this process against Variation
s in the laser intensity, laser frequency and pulse delay. Finally, we disc
uss an extension to multistate systems which provides a possibility for cre
ating coherent superpositions of more than two states.