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               228                                                                      Coherent Control of Chemical Reactions










































                      FIGURE 25 Efficiency of the transfer of population in SO 2 by STIRAP as a function of time delay between the pump
                      and Stokes laser pulses. [Reproduced with permission from Halfmann, T., and Bergmann, K. (1996). J. Chem. Phys.
                      104, 7068. Copyright American Institute of Physics.]



               molecule. In this section we show how the dipole force can     K + C 6 H 5 I → C 6 H 5 + KI  (68)
               be used to manipulate the external motion of a molecule.
                                                                 was measured by Loesch and coworkers for different ori-
               A particle with an electric dipole moment µ and a polar-
                                                                 entations of phenyl iodide. If a focusing hexapole field is
               izability α exposed to an electric field ε has a potential
                                                                 used instead of a uniform dc field, it is possible to generate
               energy
                                                                 a beam of symmetric top molecules in a single rotational
                                 1 2     2         2
               V (θ) =−µε cos θ − ε α   cos θ + α ⊥ sin θ ,  (67)  eigenstate.
                                 2
                                                                   Although the brute force method has produced many
               where θ is the angle between µ and ε, and α   and α ⊥ are  beautiful results, it is limited to molecules with a
               the parallel and perpendicular components of the polar-  permanent dipole moment and is hampered by the require-
               izability tensor, respectively. For a static electric field the  ments of high voltages, and, for a multipole focusing field,
               first term dominates, and the potential energy has a mini-  a complex apparatus. An alternate method of producing
                                                           4
               mum at θ = 0. Static field strengths on the order of 10 –  a strong electric field is to use a focused laser beam. In
                 5
               10 V/cm are typically required to align or orient a  the high frequency limit, the time average of the ac elec-
               molecule. (Alignment refers to the direction of the molec-                   2     1  2
                                                                 tric field gives 
ε(t) = 0 and 
ε (t) = 
ε  , where ε 0
                                                                                                  2  0
               ular axis without regard to which end is “up,” whereas  is the amplitude of the field. The potential energy of the
               orientation treats a molecule as a single-headed arrow.)  molecule in this case is
               For example, Wei Kong used a field strength of 58 kV/cm              1 2       2
                                                                           V (θ) =− ε  α cos θ + α ⊥ ,      (69)
               to orient a molecular beam of BrCN. This “brute force”              4 0
               method of orientation has been used to study steric ef-  where  α = α   −α ⊥ is the anisoptropy of the polarizabil-
               fects in bimolecular reactions. For example, the differen-  ity. A dimensionless quantity that is useful for scaling the
               tial cross section for the reaction               alignment of different molecules is given by
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