In this problem, we need to analyze the de Broglie wavelengths of different particles that have the same energy: a proton, a neutron, an electron, and an α-particle. The de Broglie wavelength \(\lambda\) of a particle is given by the formula:
\(\lambda = \frac{h}{p}\)
where \(h\) is Planck's constant and \(p\) is the momentum of the particle. The momentum \(p\) can be expressed in terms of mass \(m\) and velocity \(v\) as \(p = mv\).
Since the kinetic energy \(E\) is the same for all particles, we use the relationship:
\(E = \frac{1}{2}mv^2\)
Solving for velocity, we find:
\(v = \sqrt{\frac{2E}{m}}\)
Substitute this into the momentum equation:
\(p = m \sqrt{\frac{2E}{m}} = \sqrt{2mE}\)
The de Broglie wavelength then becomes:
\(\lambda = \frac{h}{\sqrt{2mE}}\)
Since all particles have the same energy \(E\), the de Broglie wavelength depends on the mass of the particles:
Thus, we consider the mass-related relationship for the wavelengths:
Thus, the correct answer is:
\(\lambda_{p} = \lambda_{n} > \lambda_{e} > \lambda_{\alpha}\)