The de-Broglie wavelength \( \lambda \) is given by: \[ \lambda = \frac{h}{p} = \frac{h}{mv} \] Where: - \( h \) is Planck's constant, - \( p \) is the momentum, - \( m \) is the mass, - \( v \) is the velocity. For an electron and a proton moving with the same velocity \( v \): \[ \lambda_e = \frac{h}{m_e v} \] \[ \lambda_p = \frac{h}{m_p v} \] The ratio of the wavelengths is: \[ \frac{\lambda_e}{\lambda_p} = \frac{m_p}{m_e} \] Thus, the ratio of de-Broglie wavelengths for the electron and proton is \( m_p: m_e \).
Final Answer: \( m_p: m_e \)

If the roots of $\sqrt{\frac{1 - y}{y}} + \sqrt{\frac{y}{1 - y}} = \frac{5}{2}$ are $\alpha$ and $\beta$ ($\beta > \alpha$) and the equation $(\alpha + \beta)x^4 - 25\alpha \beta x^2 + (\gamma + \beta - \alpha) = 0$ has real roots, then a possible value of $y$ is: