The caging of I-2 in solid Kr is followed in real-time following its d
issociative excitation on the A((3) Pi(1u)) surface. The experiments i
nvolve pump-probe measurements with a time resolution of greater than
or equal to 150 fs. The experimental signals are reproduced using clas
sical molecular dynamics simulations, and the classical Franck approxi
mation. The comparison between experiment and simulation allows an una
mbiguous interpretation of features in the observed signal as being du
e to the initial impulsive stretch of the I-I bond, collision of the a
toms with the cage wall, recoil and recombination, and the subsequent
coherent oscillations of the nascent I-2 molecule. These detailed obse
rvations are possible due to retention of coherence along the I-I coor
dinate throughout the caging process. The extent of coherence is dicta
ted mainly by the initial impact parameters of the molecule-cage colli
sion, which in turn is controlled by the thermal and zero-point amplit
udes of lattice vibrations. The caging is well-described as a sudden p
rocess, involving a binary collision between I and Kr atoms with nearl
y complete energy loss of the I atom upon completion of the first coll
ision. Vibrational relaxation of the bound molecule proceeds on the ti
me scale of 12 ps. The nontrivial relation between this relaxation tim
e and decay rates that may be extracted from experimental transients i
s discussed. Although the interplay between the nested A and A' potent
ials is not detectable, it is clear that in the studied range of initi
al excess energies, 1000-1700 cm(-1), the recombination remains effect
ively adiabatic, and does not involve the ground state.