Fig. S5.

The vDOSs at different $p$ in the 3D unstressed system. (A) Plot of the vDOSs $g(\omega )$ against the scaled frequency $\widehat{\omega }=\omega /{\omega }_{\ast }$ for several different $p$. (B) Plot of the scaled vDOSs $\widehat{g}=g(\omega )/A_0{\omega }_{\ast }^2$ against $\widehat{\omega }$. Insets are the same as the main images, but for the reduced vDOSs $g/{\widehat{\omega }}^2$ in A and $\widehat{g}/{\widehat{\omega }}^2$ in B. Around ${\omega }_{\text{BP}}={\omega }_{\ast }$, the vDOSs are collapsed onto the non-Debye scaling law $g(\omega )={\alpha }_{\text{BP}}$ ${\widehat{\omega }}^2$ with ${\alpha }_{\text{BP}}$ = 0.20.Below ${\omega }_0$ = 0.39 ${\omega }_{\ast }$, the vDOSs are collapsed onto the Debye vDOS $g(\omega )=A_0{\omega }^2$.