Concept:
De Broglie wavelength:
\[
\lambda = \frac{h}{p}
\quad,\quad p = \sqrt{2mK}
\]
So:
\[
\lambda = \frac{h}{\sqrt{2mK}}
\]
Step 1: Alpha particle and proton masses
\[
m_\alpha = 4m_p
\]
Case (i): Same kinetic energy
\[
\lambda \propto \frac{1}{\sqrt{m}}
\]
So:
\[
\frac{\lambda_\alpha}{\lambda_p}
= \sqrt{\frac{m_p}{m_\alpha}}
= \sqrt{\frac{m_p}{4m_p}}
= \frac{1}{2}
\]
\[
\boxed{\left(\frac{\lambda_\alpha}{\lambda_p}\right)_1 = \frac{1}{2}}
\]
Case (ii): Same potential difference
Kinetic energy:
\[
K = qV
\]
Alpha particle charge = $2e$, proton charge = $e$
So:
\[
K_\alpha = 2eV,\quad K_p = eV
\]
Now:
\[
\lambda = \frac{h}{\sqrt{2mK}}
\]
\[
\frac{\lambda_\alpha}{\lambda_p}
= \sqrt{\frac{m_p K_p}{m_\alpha K_\alpha}}
\]
Substitute:
\[
= \sqrt{\frac{m_p (eV)}{(4m_p)(2eV)}}
\]
\[
= \sqrt{\frac{1}{8}}
= \frac{1}{2\sqrt{2}}
\]
\[
\boxed{\left(\frac{\lambda_\alpha}{\lambda_p}\right)_2 = \frac{1}{2\sqrt{2}}}
\]
Final Answer:
\[
\text{(i) } \frac{1}{2}, \quad \text{(ii) } \frac{1}{2\sqrt{2}}
\]