Introduction to Quantum Mechanics · Problem 5.33

Identical Particles — David J. Griffiths

Physics — Quantum Mechanics · pauli_paramagnetism

Problem

Pauli paramagnetism. If the free electron gas (Section 5.3.1) is placed in a uniform magnetic field B=Bk^\mathbf{B} = B\hat{k}, the energies of the spin-up and spin-down states will be different: Enxnynz±=ℏ2π22m(nx2lx2+ny2ly2+nz2lz2)±μBB.E^{\pm}_{n_x n_y n_z} = \frac{\hbar^2 \pi^2}{2m} \left( \frac{n_x^2}{l_x^2} + \frac{n_y^2}{l_y^2} + \frac{n_z^2}{l_z^2} \right) \pm \mu_B B. There will be more spin-down states occupied than spin-up states (since they are lower in energy), and consequently the system will acquire a magnetization (see Problem 5.32). (a) In the approximation that M/μB≪ρM/\mu_B \ll \rho, find the magnetization that minimizes the total energy. Hint: Use the result of Problem 5.32(b). (b) The magnetic susceptibility is χ=μ0dMdB.\chi = \mu_0 \frac{dM}{dB}. Calculate the magnetic susceptibility for aluminum (ρ=18.1×1022\rho = 18.1 \times 10^{22} cm−3^{-3}) and compare the experimental value of 22×10−622 \times 10^{-6}.

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