A Modern Approach to Quantum Mechanics · Problem 3.3

Time Evolution — John S. Townsend

Physics — Quantum Mechanics · pauli-spin-matrices

Problem

Show that the Pauli spin matrices satisfy σiσj+σjσi=2δijI\sigma_i\sigma_j + \sigma_j\sigma_i = 2\delta_{ij}\mathbb{I}, where ii and jj can take on the values 1, 2, and 3, with the understanding that σ1=σx\sigma_1 = \sigma_x, σ2=σy\sigma_2 = \sigma_y, and σ3=σz\sigma_3 = \sigma_z. Thus for i=ji = j show that σx2=σy2=σz2=I\sigma_x^2 = \sigma_y^2 = \sigma_z^2 = \mathbb{I}, while for i≠ji \neq j show that {σi,σj}=0\{\sigma_i, \sigma_j\} = 0, where the curly brackets are called an anticommutator, which is defined by the relationship {A^,B^}≡A^B^+B^A^\{\hat{A}, \hat{B}\} \equiv \hat{A}\hat{B} + \hat{B}\hat{A}.

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