1. de-Broglie wavelength for a charged particle accelerated through potential $V$
$$ \lambda = \frac{h}{p} = \frac{h}{mv} = \frac{h}{\sqrt{2mK}} = \frac{h}{\sqrt{2mqV}} $$
Where $h$ = Planck's constant, $m$ = mass, $q$ = charge, $V$ = accelerating potential
2. For same potential difference $V$
$$ \lambda \propto \frac{1}{\sqrt{mq}} $$
So the ratio for alpha particle $(a)$ and electron $(e)$:
$$ \frac{\lambda_a}{\lambda_e} = \sqrt{\frac{m_e q_e}{m_a q_a}} $$
3. Compare masses and charges
Alpha particle = He nucleus: $m_a \approx 4m_p \approx 4 \times 1836 \, m_e \approx 7344 \, m_e$
Charge: $q_a = +2e$, while $q_e = e$
$$ m_a \gg m_e \quad \text{and} \quad q_a = 2q_e $$
$$ \frac{\lambda_a}{\lambda_e} = \sqrt{\frac{m_e \cdot e}{7344 m_e \cdot 2e}} = \sqrt{\frac{1}{14688}} \approx \frac{1}{121} $$
Therefore: $\lambda_e \gg \lambda_a$ or $\lambda_e > \lambda_a$
Electron has much larger de-Broglie wavelength than alpha particle for same accelerating voltage.
When ultraviolet rays incident on metal plate then photoelectric effect does not occur, it occurs by incidence of