According to de Broglie's hypothesis, the de Broglie wavelength \( \lambda \) of a particle is given by the equation:
\[
\lambda = \frac{h}{p}
\]
where \( h \) is Planck's constant and \( p \) is the momentum of the particle. For a particle with mass \( m \) and velocity \( v \), the momentum \( p \) is given by:
\[
p = mv
\]
Thus, the de Broglie wavelength for each particle is:
\[
\lambda_1 = \frac{h}{m_1 v_1} \quad \text{and} \quad \lambda_2 = \frac{h}{m_2 v_2}
\]
The ratio of the wavelengths is:
\[
\frac{\lambda_1}{\lambda_2} = \frac{\frac{h}{m_1 v_1}}{\frac{h}{m_2 v_2}} = \frac{m_2 v_2}{m_1 v_1}
\]
Since the initial particle is at rest, by conservation of momentum, the momentum of the two resulting particles is equal and opposite. Therefore, the momentum of each particle must satisfy:
\[
m_1 v_1 = m_2 v_2
\]
This implies:
\[
\frac{m_2 v_2}{m_1 v_1} = 1
\]
Thus, the ratio of the de Broglie wavelengths is:
\[
\frac{\lambda_1}{\lambda_2} = 1 : 1
\]