A Modern Approach to Quantum Mechanics · Problem 5.5

Wave Mechanics in One Dimension — John S. Townsend

Physics — Quantum Mechanics · electron-positron-spin-magnetic-field

Problem

At time t=0t = 0, an electron and a positron are formed in a state with total spin angular momentum equal to zero, perhaps from the decay of a spinless particle. The particles are situated in a uniform magnetic field B0B_0 in the zz direction. (a) If interaction between the electron and the positron may be neglected, show that the spin Hamiltonian of the system may be written as H^=ω0(S^1z−S^2z)\hat{H} = \omega_0(\hat{S}_{1z} - \hat{S}_{2z}) where S^1\hat{S}_1 is the spin operator of the electron, S^2\hat{S}_2 is the spin operator of the positron, and ω0\omega_0 is a constant. (b) What is the spin state of the system at time tt? Show that the state of the system oscillates between a spin-0 and a spin-1 state. Determine the period of oscillation. (c) At time tt, measurements are made of S1xS_{1x} and S2xS_{2x}. Calculate the probability that both of these measurements yield the value ℏ/2\hbar/2.

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