The colour flux on the prism
The colour flux is a vector on the colour edges. On the cube every vertex meets one z-edge, so closure forces \(b_{s}=0\) — no confining contour. The prism adds τ, opening the zτ-face, where the flux closes as the field strength Fzτ, an alternating four-cycle with \(|b_{s}|^{2}=4\).
Spectral decomposition over the edge operator
The flux spreads over the edge operator \(M_{1}=L_{1}+I\). Its projections give the propagator weight
\[ G_{b_s}=\frac{7/24}{1}+\frac{1/4}{5}+\frac{1/3}{7}+\frac{1/8}{9}=\frac{127}{315}=0.403175, \]
and the edge Sakharov trace, led by the seventeen zero-modes of the edge kernel, is
\[ \Sigma_E=\operatorname{Tr}M_1^{-1}=\frac{17}{1}+\frac43+\frac65+\frac47+\frac19=\frac{6368}{315}=20.21587, \]
\[ \Pi_{b_s}=\frac{G_{b_s}}{\Sigma_E}=\frac{127}{6368}=0.019943. \]
The master equation
The flux is a vector (p=2) carrying fundamental colour charge threading the octet, Θbs=3/8. Through the master equation with the spectral weight squared,