The fringe width \( \beta \) in a Young's double-slit experiment is given by the formula:
\( \beta = \frac{\lambda D}{d} \) where
\( \lambda \) is the wavelength of the particles (electrons or protons),
\( D \) is the distance between the slits and the screen, and
\( d \) is the slit separation.
Since the wavelength \( \lambda \) of a particle depends on its momentum, the electron, being lighter, has a longer de Broglie wavelength than the proton. Therefore, the fringe width for the electron beam \( \beta_1 \) will be greater than that for the proton beam \( \beta_2 \),
i.e., \( \beta_1 > \beta_2 \).