In this paper we study the low temperature (
T→0) behaviors of the weakly interacting Hubbard model on the honeycomb lattice with a bare chemical potential, which takes values in a small neighborhood of the renormalized chemical potential
μ, which is fixed to be
1. We prove that the two-point Schwinger's function is an analytic function of the coupling constant
λ in the domain
∣λ∣⋅∣logT∣2<1. But the ground state of this model is not a Fermi liquid, because analytic properties of self-energy don't satisfy the Salmhofer's criterion on the Fermi liquids at finite temperature.