Three matrices ,

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

Invariance, Ch Representations of Lie algebras: spin, products and SU(3)

Problem

Three 4×44\times4 matrices JxJ_x, JyJ_y, JzJ_z satisfy [Ja,Jb]=iϵabcJc[J_a,J_b] = i\epsilon_{abc}J_c. In a basis in which JzJ_z is diagonal, Jz=diag(1,0,−1,0)J_z = \mathrm{diag}(1, 0, -1, 0) and the Casimir operator is J2=diag(2,2,2,0)J^2 = \mathrm{diag}(2, 2, 2, 0). Someone argues: “Four dimensions means 2j+1=42j+1 = 4, so j=32j = \tfrac32, and J2J^2 must be 1541\tfrac{15}{4}\mathsf1. These matrices cannot satisfy the algebra.” ((a)) Find the error in this argument. ((b)) Identify the representation from the eigenvalues of J2J^2, and check your answer against the dimension and the eigenvalues of JzJ_z.

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