Fig. 2.

Microcrystallites coexisting with LFS. (A) $T_{\text{a}}$ dependence of $I\left(q\right)$ of liquid II in a small-angle regime. The scattering at $q>0.4$ ${\text{nm}}^{-1}$ comes from LFS, whereas the scattering at $q<0.4$ ${\text{nm}}^{-1}$ comes from microcrystallites. Here the slope of the Porod law $\left(I\left(q\right)\propto q^{-4}\right)$ is also indicated. (B) $T_{\text{a}}$ dependence of $I\left(q\right)$ in a wide-angle regime.