The variation of stopping potential \( (V_0) \) as a function of the frequency \( (v) \) of the incident light for a metal is shown in figure. The work function of the surface is:
\( 1.36 \, \text{eV} \)
\( 18.6 \, \text{eV} \)
\( 2.98 \, \text{eV} \)
\( 2.07 \, \text{eV} \)