In any dimension $N \geq 1$, for given mass a>0, we look to critical points of the energy functional $$I(u) = \frac{1}{2}\int_{\mathbb{R}^N}|\nabla u|^2 dx + \int_{\mathbb{R}^N}u^2|\nabla u|^2 dx - \frac{1}{p}\int_{\mathbb{R}^N}|u|^p dx$$ constrained to the set $$\mathcal{S}_a=\{ u \in X | \int_{\mathbb{R}^N}| u|^2 dx = a\},$$ where X:=\left\{u \in H^1(\mathbb{R}^N)\Big| \int_{\mathbb{R}^N} u^2|\nabla u|^2 dx <\infty\right\}. We focus on the mass super-critical case $$4+\frac{4}{N}0$when$1\leq N\leq 4$. For$N\geq 5$, we find an explicit number$a_0$such that the existence of minimizer is true if and only if$a\in (0, a_0]$. In the mass super-critical case, the existence of a minimizer to the problem $M_a$, or more generally the existence of a constrained critical point of $I$ on $\mathcal{S}_a$, had hitherto only been obtained by assuming that $p \leq 2^*$. In particular, the restriction $N \leq 3$ was necessary. We also study the asymptotic behavior of the minimizers to $M_a$ as the mass $a \downarrow 0$, as well as when $a \uparrow a^*$, where $a^*=+\infty$ for $1\leq N\leq 4$, while $a^*=a_0$ for $N\geq 5$.