A deuteron and an alpha particle having equal kinetic energy enter perpendicularly into a magnetic field. Let \( r_d \) and \( r_\alpha \) be their respective radii of circular path. The value of \( \dfrac{r_d}{r_\alpha} \) is
\( \dfrac{1}{\sqrt{2}} \)
\( 2 \)
\( 1 \)
\( \sqrt{2} \)