When a metallic surface is illuminated with radiation of wavelength \({ \lambda }\), the stopping potential is V. If the same surface is illuminated with radiation of wavelength 2\({ \lambda }\), the stopping potential is \(\frac { V }{ 4 } \) . The threshold wavelength for the metallic surface is
4\({ \lambda }\)
5\({ \lambda }\)
\(\frac { 5 }{ 2 } \)\({ \lambda }\)
3\({ \lambda }\)