“…Quantum states of a spin-j particle are described by (2j + 1) × (2j + 1) density matrices ∈ S(H) satisfying the properties † = , tr[ ] = 1, and ϕ| |ϕ 0 for all |ϕ ∈ H, dimH = 2j + 1. Taking into account the normalization condition, the density matrix is defined by (2j + 1) 2 − 1 real parameters, which are usually treated as components of the generalized Bloch vector [1,2,10,19,28]. However, many physical phenomena can be explained and visualized via a spin polarization vector p ∈ R with components p i = tr[ J i ], where J 1 , J 2 , J 3 are usual (2j + 1)-dimensional representations of angular momentum operators (see, e.g., [34]).…”