To solve this problem, we will determine the de-Broglie wavelengths for both an electron and a photon with the same energy and then find the ratio of these wavelengths.
The de-Broglie wavelength (\lambda) is given by the formula:
\lambda = \frac{h}{p}
where \( h \) is Planck's constant and \( p \) is the momentum of the particle.
For an electron, given its energy \( E \), the relation between energy and momentum is:
E = \frac{p^2}{2m}
Rearranging to find momentum \( p \), we have:
p = \sqrt{2mE}
Substituting this in the de-Broglie wavelength formula:
\lambda_e = \frac{h}{\sqrt{2mE}}
For a photon, the energy is related to momentum by:
E = pc
Solving for momentum \( p \) gives:
p = \frac{E}{c}
Substitute back into the de-Broglie formula:
\lambda_p = \frac{h}{\frac{E}{c}} = \frac{hc}{E}
The ratio of the electron's de-Broglie wavelength to the photon's de-Broglie wavelength is:
\frac{\lambda_e}{\lambda_p} = \frac{\frac{h}{\sqrt{2mE}}}{\frac{hc}{E}}
Simplifying this expression:
\frac{\lambda_e}{\lambda_p} = \frac{E}{c\sqrt{2mE}}
Further simplification gives us:
\frac{\lambda_e}{\lambda_p} = \frac{1}{c}\sqrt{\frac{E}{2m}}
The ratio of the de-Broglie wavelengths of an electron and a photon with the same energy is \frac{1}{c} \bigg( \frac{E}{2m} \bigg)^{\frac{1}{2}}. This matches option c.
