“…Using now the total z-spin component operator from (10), and applying the relations Ψ g |n d k,↑ |Ψ g = |γ 1,k | 2 + |γ 2,k | 2 + |γ 3,k | 2 , Ψ g |n d k,↓ |Ψ g = |γ 1,k | 2 + |γ 2,k | 2 + |γ 4,k | 2 , Ψ g |n f k,↑ |Ψ g = |γ 1,k | 2 + |γ 3,k | 2 + |γ 4,k | 2 , Ψ g |n f k,↓ |Ψ g = |γ 2,k | 2 + |γ 3,k | 2 + |γ 4,k | 2 ,(C5) one finds for the ground state expectation value ofŜ z per site the expression Ŝ z N sit = 1 2N sit k |γ 3,k | 2 − |γ 4,k | 2 + |γ 1,k | 2 − |γ 2,k | 2 |γ 1,k | 2 + |γ 2,k | 2 + |γ 3,k | 2 + |γ 4,k | 2 .…”