The interaction of an eta -meson with two nucleons is studied within a thre
e-body approach. The major features of the eta NN-system in the low-energy
region are accounted for by using a s-wave separable ansatz for the two-bod
y etaN and NN amplitudes. The calculation is confined to the (J(pi);T) = (0
(-);1) and (1(-);0) configurations which are assumed to be the most promisi
ng candidates for virtual or resonant eta NN-states. The eigenvalue three-b
ody equation is continued analytically into the nonphysical sheets by conto
ur deformation. The position of the poles of the three-body scattering matr
ix as a function of the etaN-intcraction strength is investigated. The corr
esponding trajectory, starting on the physical sheet, moves around the eta
NN three-body threshold and continues away from the physical area giving ri
se to virtual eta NN-states. The search for poles on the nonphysical sheets
adjacent directly to the upper rim of the real energy axis gives a negativ
e result. Thus no low-lying s-wave eta NN-resonances were found. The possib
le influence of virtual poles on the low-energy eta NN-scattering is discus
sed.