According to the photoelectric equation:
\[
E_k = h\nu - \phi
\]
where \( E_k \) is the kinetic energy of the most energetic photoelectron, \( h \) is Planck's constant, and \( \phi \) is the work function of the metal.
From de Broglie's equation for the wavelength of a particle, we have:
\[
\lambda = \frac{h}{p}
\]
where \( p \) is the momentum of the electron, and momentum \( p = \sqrt{2mE_k} \).
Substitute for \( E_k \) from the photoelectric equation:
\[
\lambda = \frac{h}{\sqrt{2m(h\nu - \phi)}}
\]
Now, replacing \( \nu \) with \( \frac{c}{\lambda} \), you will get the final expression for the de Broglie wavelength in terms of \( \phi, h, m, \) and \( \lambda \), matching option (2).
Thus, the correct answer is option (2), \( \frac{2\phi h}{h m\lambda^2} \).