Optimal control theory (OCT) is applied to laser cooling of molecules. The
objective is to cool vibrations, using shaped pulses synchronized with the
spontaneous emission. An instantaneous in time optimal approach is compared
to solution based on OCT. In both cases the optimal mechanism is found to
operate by a "vibrationally selective coherent population trapping". The tr
apping condition is that the instantaneous phase of the laser is locked to
the phase of the transition dipole moment of nu = 0 with the excited popula
tion. The molecules that reach a = 0 by spontaneous emission are then trapp
ed. while the others are continually repumped. For vibrational cooling to n
u = 2 and rotational cooling, a different mechanism operates. The field com
pletely changes the transient eigenstates of the Hamiltonian creating a sup
erposition composed of many states. Finally this superposition is transform
ed by the field to the target energy eigenstate. (C) 2001 Elsevier Science
B.V. All rights reserved.