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A paramagnetic material containing paramagnetic ions with total angular momentum \(J = \frac{1}{2}\) is kept at absolute temperature T. The ratio of the magnetic field required for 80% of the ions to be in the lowest energy state to that required for having 60% of the ions to be in the lowest energy state at the same temperature is

  • A.\(\frac{2\mathrm{ln}\, 2}{\mathrm{ln}(\frac{3}{2})}\)
  • B.\(\frac{\mathrm{ln}\, 2}{\mathrm{ln}(\frac{3}{2})}\)
  • C.\(\frac{3\mathrm{ln}\, 2}{\mathrm{ln}(\frac{3}{2})}\)
  • D.\(\frac{\mathrm{ln}\, 3}{\mathrm{ln}(\frac{3}{2})}\)

Answer: A

The ratio is \(\frac{2\ln 2}{\ln(\frac{3}{2})}\).

For \(J = \frac{1}{2}\) there are two levels at \(\mp\mu B\). With \(x = \frac{\mu B}{k_{B}T}\), the fraction in the lower level is \(\frac{1}{1 + e^{-2x}}\).

\[ \begin{aligned} 80\%: e^{-2x_{1}} &= \tfrac{1}{4} \Rightarrow x_{1} = \ln 2 \\ 60\%: e^{-2x_{2}} &= \tfrac{2}{3} \Rightarrow x_{2} = \tfrac{1}{2}\ln\tfrac{3}{2} \end{aligned} \]

At the same temperature the field is proportional to \(x\), so \(\frac{B_{1}}{B_{2}} = \frac{2\ln 2}{\ln(3/2)}\), about 3.4.

\(\frac{\ln 2}{\ln(3/2)}\) drops the factor of 2 from \(x_{2}\), and the others come from wrong occupation fractions.

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