Step 1: For equal kinetic energy \( E \), momentum is \( p = \sqrt{2mE} \), so the lighter particle carries less momentum.
Step 2: Since \( \lambda = \frac{h}{p} \), the wavelength ratio between the electron and the proton reduces to an expression in their two masses.
Step 3: Working this through gives \[ \boxed{\frac{\lambda_e}{\lambda_p} = \frac{m_e}{m_p}} \], matching option (B).