A small particle of mass \( m \) moves in such a way that its potential energy \( U = \dfrac{1}{2} m \omega^{2} r^{2} \) where \( \omega \) is constant and \( r \) is the distance of the particle from origin. Assuming Bohr’s quantization of momentum and circular orbit, the radius of \( n^{\text{th}} \) orbit will be proportional to: