The mean-squared displacement (MSD) of a hard sphere and of a dumbbell mole
cule consisting of two fused hard spheres immersed in a dense hard-sphere s
ystem is calculated within the mode-coupling theory for ideal liquid-glass
transitions. It is proven that the velocity correlator, which is the second
time derivative of the MSD, is the negative of a completely monotone funct
ion for times within the structural-relaxation regime. The MSD is found to
exhibit a large time interval for structural relaxation prior to the onset
of the cy process, which cannot be described by the asymptotic formulas for
the mode-coupling-theory-bifurcation dynamics. The ru process for molecule
s with a large elongation is shown to exhibit an anomalously wide crossover
interval between the end of the von Schweidler decay and the beginning of
normal diffusion. The diffusivity of the molecule is predicted to vary nonm
onotonically as a function of its elongation.