(b) In perpendicular magnetic field
Magnetic force = centripetal force
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ qvB = \frac{mv^{2}}{r}\ \Rightarrow r = \frac{mv}{qB}$
For proton $\ q_{1} = e,\ m_{1} = m$
For $\mathbf{\alpha}$-particle $q_{2} = 2e,\ m_{2} = 4m$
$\therefore\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \frac{r_{1}}{r_{2}} = \frac{m_{1}v}{q_{1}B}\ \times \frac{q_{2}B}{m_{2}v}$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \frac{r_{1}}{r_{2}} = \frac{m}{e}\ \times \frac{2e}{4m}$
$\ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \ \frac{r_{1}}{r_{2}} = \frac{1}{2}$