The magnetic field vector of an electromagnetic wave is given by \( \vec{B_0} = B_0 \dfrac{\hat{i} + \hat{j}}{\sqrt{2}} \cos(k z - \omega t) \); where \( \hat{i}, \hat{j} \) represents unit vector along \( x \) and \( y \)-axis respectively. At \( t = 0 \, \text{s} \), two electric charges \( q_1 \) of \( 4\pi \) coulomb and \( q_2 \) of \( 2\pi \) coulomb located at \( \left(0, 0, \dfrac{\pi}{k}\right) \) and \( \left(0, 0, \dfrac{3\pi}{k}\right) \), respectively, have the same velocity of \( 0.5\,c\,\hat{i} \), (where \( c \) is the velocity of light). The ratio of the force acting on charge \( q_1 \) to \( q_2 \) is: