The Hamiltonian of a system of two quantum mechanical particles moving on the
d-dimensional lattice Zd and interacting via zero-range attractive pair
potentials is considered. For the two-particle energy operator Hμ(K),K\in \T^d=(-\pi,\pi]^d -- the two-particle quasi-momentum, the existence of a
unique positive eigenvalue z(μ,K) above the upper edge of the essential
spectrum of Hμ(K) is proven and asymptotics for z(μ,K) are found
when μ approaches to some μ0(K) and $K\to 0.