Step 1: The probability depends on the number of available states and the magnetic moment associated with the spin. The system has three possible configurations, so the probability for each state is \( \frac{1}{3} \).
Step 2: The magnetic moment in the +z direction for the first spin is \( \frac{-1}{3} \mu \), resulting in the given configuration.
Thus, the correct answer is (A).
A system of two atoms can be in three quantum states having energies 0, $\epsilon$ and $2\epsilon$. The system is in equilibrium at temperature \( T = (k_B\beta)^{-1} \). Match the following Statistics with the Partition function.
Consider a single one-dimensional harmonic oscillator of angular frequency \( \omega \), in equilibrium at temperature \( T = \left( k_B \beta \right)^{-1 }\). The states of the harmonic oscillator are all non-degenerate having energy \( E_n = \left( n + \frac{1}{2} \right) \hbar \omega \) with equal probability, where \( n \) is the quantum number. The Helmholtz free energy of the oscillator is