Step 1: Use the photoelectric equation.
The photoelectric equation is given by:
\[
eV = h \nu - \phi
\]
where \( e \) is the charge of the electron, \( V \) is the stopping potential, \( h \) is Planck’s constant, \( \nu \) is the frequency of the light, and \( \phi \) is the work function of the material.
The frequency \( \nu \) is related to the wavelength \( \lambda \) by:
\[
\nu = \frac{c}{\lambda}
\]
where \( c \) is the speed of light.
Step 2: Calculate the change in stopping potential.
For the light of wavelength \( \lambda \), the stopping potential is \( V \). For light of wavelength \( 3\lambda \), the stopping potential is \( \frac{V}{6} \). Using the photoelectric equation, we get:
\[
eV = h \frac{c}{\lambda} - \phi
\]
\[
e \frac{V}{6} = h \frac{c}{3\lambda} - \phi
\]
By solving these two equations, we can find that the threshold wavelength is \( 5\lambda \).
Step 3: Conclusion.
Thus, the threshold wavelength for the surface is \( 5\lambda \), which corresponds to option (A).