“…Denote the spins of the three edges e 1 , e 2 , e 3 incident at v by j 1 , j 2 , j 3 . Then the part of the spin-network state T v,s γ, j, i (A) (the notation s denotes the segments s I ) corresponding to v can be expressed graphically as (see [12,13] for an introduction to the graphical method in LQG)…”