We report a unified theoretical framework for the study of the pump-du
mp control with either a single coherent field or a pair of phase-unlo
cked coherent fields in both the strong and weak response regimes, and
in terms of both the Liouville-space density matrix dynamics and the
Hilbert-space wave function evolution. Shown are also the close relati
ons between the pump-dump control kernels in the phase-locked (i.e. th
e single coherent field) and the phase-unlocked control schemes in the
strong response regime. These strong field control kernels can furthe
r be linearized in the case of pure state control in the weak pump-dum
p response regime. In this case, the optimal control theory reduces to
the eigen problem of a certain specially constructed Hermitian matrix
, from which even the globally optimal pump-dump control fields in eit
her the phase-locked or the phase-unlocked control scheme can be ident
ified. The common key quantity in both of the control schemes is a Hil
bert-space pump-dump control response function, B(tau,tau'), which sha
res a great amount of information mutually with the optical resonant R
aman spectroscopies. Numerical examples of pump-dump controlling I, vi
bration onto an eigenstate and onto a minimum uncertainty wave packet
in the ground electronic X state are presented to further elucidate th
e control mechanisms in the phase-locked and phase-unlocked schemes in
the weak response regime. (C) 1998 Elsevier Science B.V. All rights r
eserved.