We have considered a coherent population transfer to a higher excited singlet state (S2) of
molecules with anomalous fluorescence in molecular assemblies (e.g., a dense medium). A direct
excitation to S2 requires light in the UV region. Because of this, the transition is conveniently realized by a two-step (two-photon) process: S0→S1→S2, where transitions S0→S1 and S1→S2 correspond to the optical region. We have shown that efficient stimulated Raman adiabatic passage
(STIRAP) in the ladder configuration can be realized in this case, using suitably chirped pulses, to
compensate a change of the two-photon transition frequency in time, induced by the pulses themselves, due to near dipole-dipole interactions. We have provided a reduced state formulation of the
optical control process. Chirping the “pump” pulse that excites transition S0→S1 is nonequivalent to chirping the “Stokes” pulse that excites transition S1→S2, with respect to the population of the intermediate state (S1) in the pulse nonadiabatic regime. We have also shown that with suitably chirped pulses, efficient STIRAP still persists even for a rather large decay of the intermediate state.
Stimulated Raman Adiabatic Passage in a Dense Medium
