Franz Schwabl Quantum Mechanics 4th Edit · Problem 10.2

Approximation Methods for Stationary States

Physics — Quantum Mechanics · spin-half-two-particle-energy-eigenvalues

Problem

Suppose that a system consists of two distinguishable particles each with spin S=1/2S = 1/2 and is described by the Hamiltonian H=−a+b2 (S1,z+S2,z) B−a−b2 (S1,z−S2,z) B+JS1⋅S2  ,H = -\frac{a+b}{2}\,(S_{1,z} + S_{2,z})\,B - \frac{a-b}{2}\,(S_{1,z} - S_{2,z})\,B + J\mathbf{S}_1 \cdot \mathbf{S}_2 \;, where aa, bb, and JJ are constants, and BB represents the external magnetic field. Determine the energy eigenvalues.

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