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Laser snapshots of molecular motions  19



                                 eration also offers the chance to develop coherent, ultrafast X-ray laser
                                 devices.

                                 1.5.2 Coherent control of molecular dynamics
                                 When it was invented in 1960, the laser was considered by many to be the
                                 ideal tool for controlling the dynamics of molecular dissociation and colli-
                                 sions at the molecular level. The reasoning was that by choosing the fre-
                                 quency of a monochromatic (long pulse duration) laser to match exactly
                                 that of a local vibrational mode between atoms in a polyatomic molecule,
                                 it ought to be possible to deposit sufficient energy in the mode in question
                                 to bring about a massively enhanced collision probability, and thereby gen-
                                 erate a selected set of target states. With the benefit of hindsight, it is clear
                                 that the approach failed to take into account the immediate and rapid loss
                                 of mode specificity due to intramolecular redistribution of energy over a
                                 femtosecond time scale, as described above.
                                    Eight years ago it was suggested by US researchers that in order to
                                 arrive at a particular molecular destination state, the electric field asso-
                                 ciated with an ultrafast laser pulse could be specially designed to guide a
                                 molecule during a collision at different points along its trajectory in such
                                 a way that the amplitudes of all possible pathways added up coherently just
                                 along one, specific pathway at successive times after the initial photoab-
                                 sorption event. To calculate the optimal pulse shapes required by this
                                 scheme dictates the use of a so-called ‘evolutionary’ or ‘genetic’ computer
                                 algorithm to optimise, by natural selection, the electric field pattern of the
                                 laser applied to the colliding molecule at successive stages, or ‘genera-
                                 tions’, during its dynamical progress from the original progenitor state
                                 until the sought-after daughter state is maximally attained.
                                    In order that this proposal can be made to work, what is required is a
                                 device which can make rapid changes to the temporal pattern of the elec-
                                 tric field associated with a femtosecond laser pulse. The recent develop-
                                 ment of liquid-crystal spatial light modulators to act as pulse shapers
                                 fulfils this task, and may open the gateway to a plethora of experimental
                                 realisations of coherent control of molecular dynamics. There has been
                                 much theoretical work on the types of laser pulse shapes required to bring
                                 about specific molecular goals. In the laboratory, successful optical control
                                 of molecular events has been demonstrated for strategic positioning of
                                 wavepackets, enhancement of molecular ionisation probabilities, and
                                 optimisation of different photodissociation pathways. With the advent of
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