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: \[ \boxed{\text{(2) } -k^2} \]
