The equation for energy \(E\) is given as \(E = \frac{hc}{\lambda_p}\), which can be rearranged to \(\lambda_p = \frac{hc}{E}\). Using the relationship \(\lambda_n = \frac{h}{p}\), where \(p\) represents momentum, we substitute the expression for \(p\): \[\lambda_n = \frac{h}{p} = \frac{h}{\sqrt{2mE}}\] Substituting the expression for \(p\) again yields: \[\frac{\lambda_n}{\lambda_p} = \frac{\frac{h}{\sqrt{2mE}}}{\frac{h}{Ehc}} = \frac{E}{\sqrt{2mc^2}}\] This results in the expression: \[\frac{\lambda_n}{\lambda_p} = \sqrt{\frac{E}{2mc^2}}\] This provides the required expression for \(\frac{\lambda_n}{\lambda_p}\).