# Anticommutator of spin-1 matrices

We know that in the spin-1/2 representation the anticommutation relation of the Pauli matrices is $$\{\sigma_{a},\sigma_{b}\}=2\delta_{ab}I$$. Does a similar relation hold for the spin-1 representation?

For the spin 1 representation of the algebra, $$J^a_{~~bc}=-i\epsilon_{abc}$$, consisting of hermitean, imaginary, antisymmetric 3×3 matrices, i.e. the adjoint representation, it is straightforward to compute all anticommutators explicitly, $$\{J^a,J^b \}_{mk}= -\epsilon_{amn} \epsilon_{bnk} -\epsilon_{bmn}\epsilon_{ank}= 2\delta_{ab}\delta_{mk} -(\delta_{am}\delta_{bk}+\delta_{bm}\delta_{ak}).$$
• For $$a\neq b$$, they are traceless off-diagonal ones;
• For $$a=b$$, they are diagonal, traceful ones, but with a 0 in the ab entry.