Consider the normal incidence of a plane electromagnetic wave with electric field given by \[ \vec{E} = E_0 \exp{[i(k_1 z - \omega t)]} \hat{x} \] over an interface at \( z = 0 \) separating two media [wave velocities \( v_1 \) and \( v_2 \) (with \( v_2>v_1 \)) and wave vectors \( k_1 \) and \( k_2 \), respectively], as shown in the figure. The magnetic field vector of the reflected wave is 