(d) According to Einstein’s photoelectric equation
$K_{\max} = hv - \phi_{0}$
$eV_{s} = \frac{hc}{\lambda} - \phi_{0} \Rightarrow V_{s} = \frac{hc}{\lambda e} - \frac{\phi_{0}}{e}$
Where, $\lambda =$ Wavelength of incident light
$\phi_{0} =$ Work function
$V_{s} =$ Stopping potential
According to given problem
$V_{1} = \frac{hc}{\lambda e} - \frac{\phi_{0}}{e}$
$V_{2} = \frac{hc}{\left( \frac{\lambda}{2} \right)e} - \frac{\phi_{0}}{e}$
$V_{2} = \frac{2hc}{\lambda e} - \frac{\phi_{0}}{e} = \frac{2hc}{\lambda e} - \frac{2\phi_{0}}{e} + \frac{2\phi_{0}}{e} - \frac{\phi_{0}}{e}$
$= 2\left( \frac{hc}{\lambda e} - \frac{\phi_{0}}{e} \right) + \frac{\phi_{0}}{e}$
$V_{2} = 2V_{1} + \frac{\phi_{0}}{e}$ [Using (i)]
$\therefore V_{2} > 2V_{1}$