  In this paper, we consider the $L_x^2$ solution $u$ to mass critical NLS
$iu_t+\Delta u=\pm |u|^{\frac 4d} u$. We prove that in dimensions $d\ge 4$, if
the solution is spherically symmetric and is \emph{almost periodic modulo
scaling}, then it must lie in $H_x^{1+\eps}$ for some $\eps>0$. Moreover, the
kinetic energy of the solution is localized uniformly in time. One important
application of the theorem is a simplified proof of the scattering conjecture
for mass critical NLS without reducing to three enemies(see the work of
Killip-Tao-Visan, and Killip-Visan-Zhang). As another important application, we
establish a Liouville type result for $L_x^2$ initial data with ground state
mass. We prove that if a radial $L_x^2$ solution to focusing mass critical
problem has the ground state mass and does not scatter in both time directions,
then it must be global and coincide with the solitary wave up to symmetries.
Here the ground state is the unique, positive, radial solution to elliptic
equation $\Delta Q-Q+Q^{1+\frac 4d}=0$. This is the first rigidity type result
in scale invariant space $L_x^2$.
