Creation of arbitrary coherent superposition states by stimulated Raman adiabatic passage

A technique for creation of well-defined preselected coherent superpositions of multiple quantum states is proposed. It is based on an extension of the technique of stimulated Raman adiabatic passage (STIRAP) to degenerate levels. As an example, the nine-state system composed of the magnetic sublevels of three levels with angular momenta J_g=0, J_e=1, and J_f=2 is studied in detail. Starting from the ∣J_g=0,M_g=0⟩ state, STIRAP can create an arbitrary preselected coherent superposition between the five M_f sublevels (M_f=−2,−1,0,+1,+2) of the J_f=2 level with 100% efficiency in the adiabatic limit. The populations and the phases of the M_f states in this superposition are determined entirely by the polarizations of the two laser fields. It is shown that this technique allows one to create any superposition of the five M_f states, that is, to reach any point in the Hilbert space of the J_f=2 manifold, and the corresponding recipes for choosing the laser polarizations are presented.