Tdg. Walsh et al., ABOVE-THRESHOLD DISSOCIATION IN THE LONG-WAVELENGTH LIMIT, Journal of physics. B, Atomic molecular and optical physics (Print), 31(21), 1998, pp. 4853-4872
Detailed measurements of fragment kinetic energy spectra coming from t
he interaction between intense 10.6 mu m laser pulses and hydrogen and
deuterium molecules have been made. Both the proton and the deuteron
spectra exhibit a broad continuum distribution with a finer peak struc
ture superimposed. These fragments are associated with the dissociatio
n stage of the interaction. The broad continuum is understood using a
simple two-step model in which the first stage involves the barrier-su
ppression dissociation of the molecular ion followed by a second step
involving the interaction between the dissociated, charged fragment an
d the electric held. This model is analogous to the 'Simpleman theory'
(van Linden van den Heuvell and Muller 1988 Multiphoton Processes, Ca
mbridge Studies in Modern Optics vol 8 ed S J Smith and P L Knight (Ne
w York: Cambridge University Press)) which has been used in the interp
retation of long-wavelength above-threshold ionization results (Gallag
her 1988 Phys. Rev. Lett. 61 2304, Corkum et al 1989 Phys. Rev. Lett.
62 1259). The fine peak structure is related to the above-threshold di
ssociation picture. The deuteron spectra also contain a set of higher-
energy fragments which are associated with a secondary, enhanced ioniz
ation process. The absence of corresponding higher-energy protons can
be understood in the context of the proposed two-step dissociation mod
el. The experimental spectra are also compared with the results of bot
h quantum and semiclassical calculations; these agree qualitatively we
ll.