The de-Broglie wavelength is given by:
\[
\lambda = \frac{h}{\sqrt{2mE}},
\]
where \( h \) is Planck's constant, \( m \) is the mass of the particle, and \( E \) is its energy.
For particles with the same energy, \( \lambda \propto \frac{1}{\sqrt{m}} \).
The masses of the particles are:
Electron (\( m_e \)): least mass,
Proton (\( m_p \)): greater mass,
Alpha particle (\( m_\alpha = 4m_p \)): greatest mass.
Since \( \lambda \propto \frac{1}{\sqrt{m}} \), the order of the wavelengths is:
\[
\lambda_e>\lambda_p>\lambda_\alpha.
\]
\[
\boxed{\lambda_\alpha<\lambda_p<\lambda_e}
\]