Abstract This paper concerns the scalar field equation -Δu=λu+|u|q-2u+a|u|4u+b(I2∗|u|5)|u|3uin ℝ3 -\Delta u=\lambda u+|u|^{q-2}u+a|u|^{4}u+b(I_{2}\ast|u|^{5})|u|^{3}u\quad\text% {in }\mathbb{R}^{3} under the normalized constraint ∫ℝ3u2𝑑x=c2 {\int_{\mathbb{R}^{3}}u^{2}\,dx=c^{2}} , where a,b,c>0 {a,\,b,\,c>0} , 2<q<103 {2<q<\frac{10}{3}} and I2 {I_{2}} is the Riesz potential. We prove that for small prescribed mass c the above equation has a positive ground state solution and an infinite sequence of normalized solutions with negative energies tending to zero. Asymptotic properties of ground state solutions as a→0+ {a\to 0^{+}} and as b→0+ {b\to 0^{+}} are also studied.