The two-body T-matrix is calculated directly as function of two vector
momenta for different Malfliet-Tjon-type potentials. At a few hundred
MeV projectile energy the total amplitude is quite a smooth function
showing only a strong peak in forward direction. In contrast, the corr
esponding partial-wave contributions, whose number increases with incr
easing energy, become more and more oscillatory with increasing energy
. The angular and momentum dependence of the full amplitude is studied
and displayed on as well as off the energy shell as function of posit
ive and negative energies. The behaviour of the T-matrix in the vicini
ty of bound-state poles and resonance poles in the second energy sheet
is studied. It is found that the angular dependence of T exhibits ver
y characteristic properties in the vicinity of those poles, which are
given by the Legendre function corresponding to the quantum number eit
her of the bound stale or the resonance (or virtual) state. This behav
iour is illustrated along numerical examples.