Page 18 - Visions of the Future Chemistry and Life Science
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8  G. ROBERTS


































                               Figure 1.3. Real-time femtosecond spectroscopy of molecules can be described in
                               terms of optical transitions excited by ultrafast laser pulses between potential
                               energy curves which indicate how different energy states of a molecule vary with
                               interatomic distances. The example shown here is for the dissociation of iodine
                               bromide (IBr). An initial pump laser excites a vertical transition from the potential
                               curve of the lowest (ground) electronic state V to an excited state V . The
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                               fragmentation of IBr to form I Br is described by quantum theory in terms of a
                               wavepacket which either oscillates between the extremes of V or crosses over
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                               onto the steeply repulsive potential V  leading to dissociation, as indicated by the
                                                          1
                               two arrows. These motions are monitored in the time domain by simultaneous
                               absorption of two probe-pulse photons which, in this case, ionise the dissociating
                               molecule.


                                  An initial, ultrafast ‘pump’ pulse promotes IBr to the potential energy
                               curve V , where the electrostatic nuclear and electronic forces within the
                                     1
                               incipient excited IBr* molecule act to force the I and Br atoms apart. V
                                                                                           1
                               contains a minimum, however, so as the atoms begin to separate the mole-
                               cule remains trapped in the excited state unless it can cross over onto the
                               repulsive potential V , which intersects the bound curve at an extended
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