Step 1: Apply the operator \( \frac{d^2}{dx^2} \) to the wave function. First, compute the first derivative of \( \psi \): \[ \frac{d}{dx} (A e^{ikx} + B e^{-ikx}) = A ik e^{ikx} - B ik e^{-ikx} \] Next, 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. We have \( \frac{d^2}{dx^2} \psi = - k^2 \psi \). This shows that \( \psi \) is an eigenfunction with eigenvalue \( -k^2 \). Thus, the correct answer is \( -k^2 \).
Final Answer: \[ \boxed{\text{(2) } -k^2} \]
Two projectile protons \( P_1 \) and \( P_2 \), both with spin up (along the \( +z \)-direction), are scattered from another fixed target proton \( T \) with spin up at rest in the \( xy \)-plane, as shown in the figure. They scatter one at a time. The nuclear interaction potential between both the projectiles and the target proton is \( \hat{\lambda} \vec{L} \cdot \vec{S} \), where \( \vec{L} \) is the orbital angular momentum of the system with respect to the target, \( \vec{S} \) is the spin angular momentum of the system, and \( \lambda \) is a negative constant in appropriate units. Which one of the following is correct?


