A simple harmonic oscillator of angular frequency `2 "rad" s^(-1)` is acted upon by an external force `F = sint N`. If the oscillator is at rest in its equilibrium position at `t = 0`, its position at later times is proportional to :-
A. `sin t - 1/2 sin 2t`
B. `sin t + 1/2 cos 2t`
C. `sin t + 1/2 sin 2t`
D. `cos t - 1/2 sin 2t`