The period of a particle undergoing simple harmonic motion (SHM) is \(T\).

The ratio \(\frac{{{\text{acceleration of the particle}}}}{{{\text{displacement of the particle from its equilibrium position}}}}\) is proportional to

A.     \({T^{ - 2}}\).

B.     \({T^{ - 1}}\).

C.     \(T\).

D.     \({T^2}\)

A