Step 1: Use the de-Broglie wavelength formula.
The de-Broglie wavelength \( \lambda \) is given by:
\[
\lambda = \frac{h}{p}
\]
where:
- \( h \) is Planck's constant,
- \( p \) is the momentum of the particle, which is related to its mass \( m \) and velocity \( v \) by:
\[
p = mv.
\]
Step 2: Relate the kinetic energy to the velocity.
The kinetic energy \( E_k \) of a particle is given by:
\[
E_k = \frac{1}{2} mv^2.
\]
Rearranging for velocity \( v \), we get:
\[
v = \sqrt{\frac{2 E_k}{m}}.
\]
Step 3: Compare the de-Broglie wavelengths.
The de-Broglie wavelength is then:
\[
\lambda = \frac{h}{m \sqrt{\frac{2 E_k}{m}}} = \frac{h}{\sqrt{2 m E_k}}.
\]
Since both particles have the same kinetic energy, \( E_k \), the ratio of their wavelengths will depend on their masses:
\[
\frac{\lambda_1}{\lambda_2} = \sqrt{\frac{m_2}{m_1}} = \sqrt{\frac{6}{3}} = \sqrt{2}.
\]
Step 4: Conclusion.
Therefore, the ratio of the de-Broglie wavelengths is \( \lambda_1 : \lambda_2 = \sqrt{2} : 1 \), and the correct answer is option (C).