Ad. Bandrauk, MOLECULAR MULTIPHOTON TRANSITIONS - COMPUTATIONAL SPECTROSCOPY FOR PERTURBATIVE AND NONPERTURBATIVE REGIMENS, International reviews in physical chemistry, 13(1), 1994, pp. 123-161
The total Schrodinger equation for an electromagnetic field interactin
g with a molecule is shown to lead to time independent or time depende
nt coupled differential equations. The time independent equations resu
lt from using a quantized representation, i.e., photon number states,
of the electromagnetic field. The stationary states of such a quantize
d field-molecule system are called dressed states. Appropriate numeric
al methods are presented in order to treat radiative and non-radiative
interactions simultaneously for any coupling strength, i.e. from the
perturbative, Fermi-Golden rule limit, to the non-perturbative regime
for both types of interactions. Both bound-bound, bound-continuum and
continuum-continuum radiative and non-radiative transitions can be tre
ated exactly in the present scheme. The relationship between the quant
ized time independent approach and the time dependent semiclassical fi
eld method is achieved through consideration of the coherent states of
the quantized radiation field. In this limit, multiphoton transitions
are more conveniently treated by coupled partial differential equatio
ns both in time and space. The time dependent approach is therefore mo
re appropriate for very short laser pulses, especially for pulse time
durations less than the molecular natural time-scales, in which case s
tationary states are ill-defined. Examples of both time-independent an
d time dependent calculations are presented. In the first case, cohere
nt laser control of multiphoton transitions is illustrated by a time i
ndependent, all state, coupled equations method. Finally, high intensi
ty direct photodissociation by subpicosecond pulses is presented as an
example of laser pulse effects from a time dependent calculation in t
he non-perturbative regime, where laser-induced avoided crossings can
be created by the pulse itself. The coupled equations methods are in p
rinciple exact and can be readily implemented for diatomics and triato
mics with current computer technology.