Mirror Symmetry of Spencer-Hodge Decompositions in Constrained Geometric Systems: Selected Collisions and Weyl Splittings
We formulate mirror symmetry for compatible principal-bundle systems with a genuinely graded polynomial Spencer complex. Exact parity identifies its Hodge spectra, while gauge implementation is governed by eigenbundle transport. For parameterized families, a spectral coefficient extension realizes the eigenline incidence as its projectivized harmonic zero modes. A relative symplectic suspension separates scalar curvature from flag energy. On a fixed spatial bundle, mixed-Chern orthogonality constrains parameter-sphere charges; a nonzero two-band charge precludes contactness over a closed base. This incidence viewpoint organizes three kinds of spectral degeneration. Continuous diagonalization across an arbitrary closed nowhere-dense collision set is controlled by flag extension, permutation monodromy, and eigenline Chern classes. Smooth flat gaps can conceal flag behavior from every jet; polynomial gaps yield finite-jet semialgebraic blow-ups. Local Dirichlet minimality then selects a rigid cone. We classify the minimizing radial cones into every $\mathbb{C}P^N$: the nonconstant links are isometric projective-line hedgehogs. This gives projective singular-measure stability and, together with a Grassmannian degree bound, power convergence at all three-dimensional minimizing singularities in these targets. For complexified four-band pencils the same incidence is read through geometric-rank minors, giving complex isolation and a degree-twenty translation cover in a crystalline model. For every spin, jointly polynomial Hermitian unfoldings attain both universal Weyl-point count bounds; constant spin-$3/2$ translations have two sixteen-point chambers with different gap distributions. Throughout, eigenflags and geometric rank retain information absent from the scalar characteristic polynomial.