The de Broglie wavelength \( \lambda \) of a particle is related to its momentum \( p \) by the equation:
\[
\lambda = \frac{h}{p}
\]
Where:
- \( h \) is Planck's constant,
- \( p \) is the momentum of the particle.
Momentum is related to the kinetic energy \( K \) and mass \( m \) by the equation:
\[
K = \frac{p^2}{2m}
\]
Thus, the momentum can be expressed as:
\[
p = \sqrt{2mK}
\]
The de Broglie wavelength then becomes:
\[
\lambda = \frac{h}{\sqrt{2mK}}
\]
Now, we are told that the kinetic energy of the alpha particle is four times that of the proton:
\[
K_\alpha = 4K_p
\]
The ratio of the de Broglie wavelengths is:
\[
\frac{\lambda_\alpha}{\lambda_p} = \frac{\frac{h}{\sqrt{2m_\alpha K_\alpha}}}{\frac{h}{\sqrt{2m_p K_p}}}
\]
Simplifying this expression:
\[
\frac{\lambda_\alpha}{\lambda_p} = \frac{\sqrt{2m_p K_p}}{\sqrt{2m_\alpha K_\alpha}} = \frac{\sqrt{m_p K_p}}{\sqrt{m_\alpha K_\alpha}}
\]
Since the mass of the alpha particle is four times that of the proton \( m_\alpha = 4m_p \), and \( K_\alpha = 4K_p \), we get:
\[
\frac{\lambda_\alpha}{\lambda_p} = \frac{\sqrt{m_p \cdot K_p}}{\sqrt{4m_p \cdot 4K_p}} = \frac{\sqrt{m_p K_p}}{\sqrt{16 m_p K_p}} = \frac{1}{4}
\]
Thus, the ratio of the de Broglie wavelengths is \( \frac{1}{4} \). Therefore, the correct answer is option (C).