In simple harmonic motion, the time taken to move from extreme position to half the amplitude is \( t_1 \), which corresponds to a quarter of the period \( T \) of the oscillation. The time taken to move from mean position to half of the amplitude is \( t_2 \), which corresponds to half the period \( T \).
Therefore, we can conclude:
\[
t_1 = 2 t_2
\]
Thus, the correct answer is:
\[
\boxed{t_1 = 2 t_2}
\]