The existence of bound states in a system of three particles in an optical lattice

We consider the hamiltonian $\mathrm{H}_{\mu},\mu\in \R$ of a system of three-particles (two identical fermions and one different particle) moving on the lattice ${\Z}^d ,\, d=1,2 $ interacting through repulsive $(\mu>0)$ or attractive $(\mu<0)$ zero-range pairwise potential $\mu V$. We prove for any $\mu\ne0$ the existence of bound state of the discrete three-particle Schr\"odinger operator $H_{\mu}(K),\,K\in \T^d$ being the three-particle quasi-momentum, associated to the hamiltonian $\mathrm{H}_{\mu}$.