The spin rotation operator for spin one-half about a unit axis is

PHYSICS · Multi-part · Fermi University Physics · Mathematical Methods for Physics · Quantum Mechanics · Symmetry, angular momentum and spin

The Structure of Quantum Mechanics, Ch Spin one-half, SU(2) and two-level dynamics

Problem

The spin rotation operator for spin one-half about a unit axis n^\hat n is R^(n^,θ)=e−iθn^⋅σ⃗/2\hat{\mathcal R}(\hat n,\theta) = e^{-i\theta\hat n\cdot\vec\sigma/2}, where σ⃗=(σx,σy,σz)\vec\sigma = (\sigma_x,\sigma_y,\sigma_z) are the Pauli matrices. Using only the fact that (n^⋅σ⃗)2=1(\hat n\cdot\vec\sigma)^2 = \mathbb 1, which follows from the Pauli algebra, derive a closed form for R^(n^,θ)\hat{\mathcal R}(\hat n,\theta) by summing its Taylor series in θ\theta. ((a)) Give the closed form. ((b)) Evaluate R^(n^,2π)\hat{\mathcal R}(\hat n, 2\pi) and R^(n^,4π)\hat{\mathcal R}(\hat n,4\pi) for an arbitrary axis n^\hat n, writing each as a number times 1\mathbb 1. ((c)) In SO(3)SO(3), the matrix that rotates an ordinary three-dimensional vector by 2π2\pi about any axis is the identity, and so is the one for 4π4\pi. Reconcile this with your result in part (b), and state in one sentence what it tells you about the map from SU(2)SU(2) to SO(3)SO(3).

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