Concept:
The de Broglie wavelength of a particle is given by:
\[
\lambda = \frac{h}{p}
\]
For a charged particle accelerated through a potential difference \(V\), its kinetic energy is:
\[
KE = qV = \frac{1}{2}mv^2
\]
Thus, momentum \(p = \sqrt{2mqV}\), and hence:
\[
\lambda = \frac{h}{\sqrt{2mqV}}
\]
Therefore,
\[
\lambda \propto \frac{1}{\sqrt{mq}}
\]
Step 1: {Write proportional relation.}
\[
\lambda \propto \frac{1}{\sqrt{mq}}
\]
Step 2: {Substitute values for proton.}
For proton:
\[
m_p = m, \quad q_p = e
\]
\[
\lambda_p \propto \frac{1}{\sqrt{me}}
\]
Step 3: {Substitute values for alpha particle.}
For alpha particle:
\[
m_\alpha = 4m, \quad q_\alpha = 2e
\]
\[
\lambda_\alpha \propto \frac{1}{\sqrt{(4m)(2e)}} = \frac{1}{\sqrt{8me}}
\]
Step 4: {Find the ratio.}
\[
\frac{\lambda_p}{\lambda_\alpha}
=
\frac{\frac{1}{\sqrt{me}}}{\frac{1}{\sqrt{8me}}}
=
\sqrt{8}
= 2\sqrt{2}
\]
Thus,
\[
\lambda_p : \lambda_\alpha = 2\sqrt{2} : 1
\]
Approximating to given options:
\[
\lambda_p : \lambda_\alpha \approx 1 : 2
\]