Step 1: Understanding the Potential
The potential in the given system is a Dirac delta function located at \( x = a \). The delta function potential is given by:
\[ V(x) = -V_0 \delta(x-a) \] where \( V_0 \) is a positive constant and \( \delta(x-a) \) is the Dirac delta function centered at \( x = a \).
Step 2: Schrödinger Equation for the System
The Schrödinger equation for a particle under this potential is given by:
\[ -\frac{\hbar^2}{2m} \frac{d^2 \psi(x)}{dx^2} + V(x) \psi(x) = E \psi(x) \]
Substituting the given potential into the Schrödinger equation, we get: \[ -\frac{\hbar^2}{2m} \frac{d^2 \psi(x)}{dx^2} - V_0 \delta(x-a) \psi(x) = E \psi(x) \] For bound states, we expect that \( E < 0 \) (since bound states have negative energy). Let \( E = -\epsilon \), where \( \epsilon > 0 \).
Step 3: Behavior of the Wavefunction The solution to this equation can be divided into two regions: - For \( x \neq a \), the potential is zero, and the solution to the Schrödinger equation is: \[ \psi(x) = A e^{-\kappa |x-a|} \] where \( \kappa = \frac{\sqrt{2m\epsilon}}{\hbar} \). - At \( x = a \), the wavefunction will have a discontinuity due to the delta function. This discontinuity is found by integrating the Schrödinger equation around \( x = a \).
Step 4: Discontinuity in the Derivative of the Wavefunction Integrating the Schrödinger equation around \( x = a \), we find that the derivative of the wavefunction has a discontinuity: \[ \psi'(a^+) - \psi'(a^-) = -\frac{2mV_0}{\hbar^2} \psi(a) \] For a bound state to exist, the wavefunction must satisfy the condition that the discontinuity in the derivative is non-zero. This condition can only be satisfied if there is exactly one bound state, as the delta function potential creates a single bound state.
Conclusion: Since the potential \( V(x) = -V_0 \delta(x-a) \) is a single delta function, it can support only one bound state. Therefore, the number of bound states is:
\( 1 \)
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?

Find the region that represents those rural students who are not intelligent?

In the following Venn diagram, which of the following represents the educated men but not urban? 