A new formalism for the optimal control of quantum mechanical physical
observables is presented. This approach is based on an analogous classical
control technique reported previously[J. Botina, H. Rabitz and N. Rahman, J.
chem. Phys. Vol. 102, pag. 226 (1995)]. Quantum Lagrange multiplier functions
are used to preserve a chosen subset of the observable dynamics of interest. As
a result, a corresponding small set of Lagrange multipliers needs to be
calculated and they are only a function of time. This is a considerable
simplification over traditional quantum optimal control theory[S. shi and H.
Rabitz, comp. Phys. Comm. Vol. 63, pag. 71 (1991)]. The success of the new
approach is based on taking advantage of the multiplicity of solutions to
virtually any problem of quantum control to meet a physical objective. A family
of such simplified formulations is introduced and numerically tested. Results
are presented for these algorithms and compared with previous reported work on
a model problem for selective unimolecular reaction induced by an external
optical electric field.Comment: Revtex, 29 pages (incl. figures