\( \lambda_{\alpha} < \lambda_{p} < \lambda_{e} \)
\( \lambda_{\alpha} > \lambda_{p} > \lambda_{e} \)
\( \lambda_{\alpha} = \lambda_{p} = \lambda_{e} \)
\( \lambda_{\alpha} > \lambda_{p} < \lambda_{e} \)
To solve the given problem, let's first understand the relationship between De-Broglie wavelength and kinetic energy:
The De-Broglie wavelength \(\lambda\) of a particle is given by the formula:
\(\lambda = \frac{h}{p}\)
where \(\lambda\) is the De-Broglie wavelength, \(h\) is Planck's constant, and \(p\) is the momentum of the particle. The momentum \()\) can be expressed in terms of kinetic energy \((K)\) a\)
\(p = \sqrt{2mK}\)
Thus, substituting for \(p\), we have:
\(\lambda = \frac{h}{\sqrt{2mK}}\)
Given that the kinetic energy \(K\) is the same for all particles (an \(\alpha\)-particle, a proton, and an electron), the De-Broglie wavelength depends on the mass \(m\) of the particle.
Since the mass \(m\) appears in the denominator, a larger mass results in a shorter wavelength.
Let's compare the masses of the particles:
Since the \(\alpha\)-particle has the largest mass, it will have the smallest De-Broglie wavelength. Conversely, the electron, with the smallest mass, will have the largest De-Broglie wavelength.
Thus, the order of wavelengths is: \(\lambda_{\alpha} < \lambda_{p} < \lambda_{e}\).
Therefore, the correct option is:
\((\lambda_{\alpha} < \lambda_{p} < \lambda_{e})\)