Photons of wavelength $\lambda$ are incident on the cathode of a photocell. Electrons are emitted from the cathode surface. The de-Broglie wavelength of the emitted electrons (work function is negligible) is
$\left(c = \text{velocity of light},\; h = \text{Planck’s constant},\; m = \text{mass of electron}\right)$
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If work function is negligible, entire photon energy converts into kinetic energy.
Step 1: Energy of incident photon.
\[
E = \frac{hc}{\lambda}
\]
Step 2: Kinetic energy of emitted electron.
Since work function is negligible:
\[
K = \frac{hc}{\lambda}
\]
Step 3: de-Broglie wavelength of electron.
\[
\lambda_e = \frac{h}{\sqrt{2mK}}
\]
Step 4: Substituting $K$.
\[
\lambda_e = \frac{h}{\sqrt{2m\left(\frac{hc}{\lambda}\right)}} = \sqrt{\frac{h\lambda}{2mc}}
\]
Step 5: Conclusion.
The de-Broglie wavelength is $\sqrt{\dfrac{h\lambda}{2mc}}$.