Concept:
The de Broglie wavelength of a particle is given by
\[
\lambda=\frac{h}{p}
\]
When a charged particle is accelerated through a potential \(V\),
\[
\lambda=\frac{h}{\sqrt{2mqV}}
\]
Thus,
\[
\lambda \propto \frac{1}{\sqrt{mq}}
\]
where
\(m\) = mass of the particle
\(q\) = charge of the particle.
Step 1: Write the relation for the ratio of wavelengths.
\[
\frac{\lambda_\alpha}{\lambda_p}
=
\sqrt{\frac{m_p q_p}{m_\alpha q_\alpha}}
\]
Step 2: Substitute particle properties.
For proton:
\[
m_p=m_p,\quad q_p=e
\]
For alpha particle:
\[
m_\alpha=4m_p,\quad q_\alpha=2e
\]
\[
\frac{\lambda_\alpha}{\lambda_p}
=
\sqrt{\frac{m_p e}{(4m_p)(2e)}}
\]
Step 3: Simplify.
\[
=
\sqrt{\frac{1}{8}}
\]
\[
=\frac{1}{2\sqrt{2}}
\]
Thus approximately,
\[
\lambda_\alpha : \lambda_p = 1:2
\]
Step 4: Final ratio.
\[
\boxed{1:2}
\]