In this paper, we consider the Chern-Simons-Schrödinger system
{−Δu+[e2|A|2+(V(x)+2eA0)+2(1+κq2)N]u+q|u|p−2u=0,−ΔN+κ2q2N+q(1+κq2)u2=0,κ(∂1A2−∂2A1)=−eu2,∂1A1+∂2A2=0,κ∂1A0=e2A2u2,κ∂2A0=−e2A1u2,(P)
where
u∈H1(R2),
p∈(2,4),
Aα:R2→R are the components of the gauge potential
(α=0,1,2),
N:R2→R is a neutral scalar field,
V(x) is a potential function, the parameters
κ,q>0 represent the Chern-Simons coupling constant and the Maxwell coupling constant, respectively, and
e>0 is the coupling constant. In this paper, the truncation function is used to deal with a neutral scalar field and a gauge field in the Chern-Simons-Schrödinger problem. The ground state solution of the problem (P) is obtained by using the variational method.