To determine the proportionality of \(\frac{\lambda_{\mathrm{photon}}}{\lambda_{\mathrm{electron}}}\) with respect to energy \(E\), we need to analyze the wavelength expressions for both photons and electrons.
- For a photon, the energy is related to its wavelength by the equation: \(E = \frac{hc}{\lambda_{\mathrm{photon}}}\) , where \(h\) is Planck's constant and \(c\) is the speed of light.
- Rearranging gives the wavelength of the photon: \(\lambda_{\mathrm{photon}} = \frac{hc}{E}\).
- For an electron, we use the de Broglie wavelength equation: \(\lambda_{\mathrm{electron}} = \frac{h}{p}\), where \(p\) is the momentum of the electron.
- Since energy \(E\) is equal for both, the electron's energy is given by: \(E = \frac{p^2}{2m}\) (non-relativistic case).
- Solving for momentum \(p\) gives: \(p = \sqrt{2mE}\), thus the de Broglie wavelength becomes: \(\lambda_{\mathrm{electron}} = \frac{h}{\sqrt{2mE}}\).
- Now comparing \(\frac{\lambda_{\mathrm{photon}}}{\lambda_{\mathrm{electron}}}\): \(\frac{\lambda_{\mathrm{photon}}}{\lambda_{\mathrm{electron}}} = \frac{\frac{hc}{E}}{\frac{h}{\sqrt{2mE}}} = \frac{c\sqrt{2mE}}{E}\).
- After simplification, it becomes: \(\frac{\lambda_{\mathrm{photon}}}{\lambda_{\mathrm{electron}}} \propto \frac{1}{\sqrt{E}}\).
Hence, the correct answer is that \(\frac{\lambda_{\mathrm{photon}}}{\lambda_{\mathrm{electron}}}\) is proportional to \(\frac{1}{\sqrt{E}}\).