Step 1: Apply the operator \( \frac{d^2}{dx^2} \) to the wave function. Compute the first derivative of \( \psi \): \[ \frac{d}{dx} (A e^{ikx} + B e^{-ikx}) = A ik e^{ikx} - B ik e^{-ikx} \] Compute the second derivative: \[ \frac{d^2}{dx^2} (A e^{ikx} + B e^{-ikx}) = - A k^2 e^{ikx} - B k^2 e^{-ikx} \] \[ = - k^2 (A e^{ikx} + B e^{-ikx}) \]
Step 2: Interpret the result. The result is \( \frac{d^2}{dx^2} \psi = - k^2 \psi \). This indicates that \( \psi \) is an eigenfunction with eigenvalue \( -k^2 \). Therefore, the eigenvalue is \( -k^2 \).
Final Answer: \[ \boxed{\text{(2) } -k^2} \]
A beam of light of wavelength \(\lambda\) falls on a metal having work function \(\phi\) placed in a magnetic field \(B\). The most energetic electrons, perpendicular to the field, are bent in circular arcs of radius \(R\). If the experiment is performed for different values of \(\lambda\), then the \(B^2 \, \text{vs} \, \frac{1}{\lambda}\) graph will look like (keeping all other quantities constant).