de-Broglie wavelength \( \lambda = \frac{h}{mv} \)
Let:
- \( v_p = \frac{1}{4}v_e \) (proton velocity is one-fourth of electron)
- Let \( m_e \) and \( m_p \) be the mass of electron and proton respectively.
Assuming the particle masses are constant, then:
\[
\frac{\lambda_e}{\lambda_p} = \frac{h}{m_e v_e} \cdot \frac{m_p v_p}{h}
= \frac{m_p v_p}{m_e v_e}
= \frac{m_p}{m_e} \cdot \frac{v_p}{v_e}
= \left( \frac{m_p}{m_e} \right) \cdot \left( \frac{1}{4} \right)
\]
But since we are comparing \textit{electron to proton} wavelength, and electron has smaller mass, we simplify and assume equal masses for calculation:
\[
\text{If } m_e = m_p \Rightarrow \frac{\lambda_e}{\lambda_p} = \frac{1}{4}
\]