The magnitude peak near $\omega_n\!\approx\!100$ rad/s indicates a lightly damped 2nd-order low-pass:
$\dfrac{10000}{s^2+2s+10000}$ (since $2\zeta\omega_n=2\Rightarrow \zeta\approx0.01$ gives a tall resonance).  
Options (A) and (B) share this magnitude. The plotted phase, however, decreases far beyond $-180^\circ$ (approaching about $-700^\circ$ by 200 rad/s), which requires an additional frequency-proportional lag. A pure time delay $e^{-0.05s}$ contributes phase $-\omega(0.05)$ (radians), matching the observed extra linear drop. Hence (B).