Step 1: The given state \( | \phi \rangle \) is a superposition of spin states. To find the probability of measuring \( S_x = + \hbar/2 \), we project the state onto the eigenstate of \( S_x \).
Step 2: The probability is given by the square of the absolute value of the overlap between \( | \phi \rangle \) and the \( S_x = + \hbar/2 \) eigenstate. Using the properties of spin-1/2 particles and the normalization, we calculate:
\[
P(S_x = + \hbar/2) = \left| \langle + | \phi \rangle \right|^2 = \frac{17}{18}
\]
Thus, the correct answer is (D).
| Column I | Column II |
(1)![]() | (P) Diamagnetic |
(2)![]() | (Q) Paramagnetic |
(3)![]() | (R) Ferromagnetic |
(4)![]() | (S) Antiferromagnetic |
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?
