We investigate solution behavior with an emphasis on the localization of a
double chain built up from two coupled one-dimensional Ablowitz-Ladik (AL)
lattices. Whereas each one-dimensional AL lattice is completely integrable,
the AL-type coupling between them causes the system to become nonintegrabl
e. With regard to the stationary system we present a rigorous proof of its
nonintegrability by means of the Melnikov method. Concerning stationary loc
alized states, we identify the parameter regions for which the origin of th
e stationary map represents a hyperbolic equilibrium point. We show the exi
stence of transversal intersections of the stable and unstable manifolds of
the hyperbolic point. The associated homoclinic orbit is used to excite st
anding bright two-soliton-like excitations on the double chain. We compute
both, analytically as well as numerically, the dynamical energy exchange ra
te between the two AL strings when on each of them a single AL soliton is l
aunched. It is shown that the soliton interaction depends on the distance b
etween the solitons and their mutual phase relation. There exist distinct e
nergy exchange regimes ranging from suppressed to pronounced energy exchang
e. In the latter case directed energy flow from one chain into the other ta
kes place. Eventually almost all energy is stored in a single chain in the
form of a breather solution showing a bias toward one-dimensional coherent
excitation patterns. In general, the single solitons from the integrable li
mit with no mutual coupling survive as moving breathers under the action of
the nonintegrable coupling, and thus experience no lattice pinning. The on
ly pinned solution we obtained resulted from the homoclinic orbit derived f
rom the stationary system. As an interesting dynamical feature we observe t
hat a single soliton may split into two moving breathing states of differen
t amplitudes as well as different velocities.