Four harmonics of equal frequencies and equal intensities \(I_{0}\) have phase angles \(0,\frac{\pi }{3},\frac{2\pi }{3},\pi\). When they are superimposed, the intensity of the resultant wave is "\(nI_{0}\)". The value of n is
(all phase angles are in radian and \(\cos (60)^{\circ }=\frac{1}{2}\))