Discrete induction and its open interfaces [fdip-003W]

How can algebra and geometry organize induction and background variation? Gaussian elimination gives a finite example; the synthesis conjecture and finite interfaces distinguish this result from the further maps required.

The route through these explorations is the diagram opening the compatibility test. That test fixes one finite spinor datum. The larger proposals remain open tests. The conjecture and finite interfaces below remain distinct from those open questions.

The constructions now on this route include finite-group symmetry, selected backgrounds and connections, finite and compact gauge fields, reflection positivity, explicit transfer operators, Gauss's law, Grassmann integration, fermionic elimination, the covariant Dirac operator and the free Wilson remedy. The arrow from gauge fields to Euclidean time, drawn in the reader guide, is a reading prerequisite for the gauge transfer and for Gauss's law. Reflection positivity alone does not supply that time shift. The arrow from gauge fields to lattice fermions is a reading prerequisite for the covariant Dirac operator and for the free Wilson remedy that follows it, not for Grassmann integration or fermionic elimination, and not an identification of those operators with a physical electron.

The comparisons that remain open are these. The physical environment map \(E\) is not constructed. The supplied-circle limit controls one fixed Fourier mode; it is not a continuum limit of the full induced law, and no moduli map controls that limit. The enriched background groupoid and the geometric realization do not supply a site, a stack, or a descent that organizes those families. The larger proposals remain open tests. What the structure fixes and what it leaves free records that comparison. The chapters transcluded by Structure develop the questions of that part. None of these absences is a no-go theorem or a physical identification.

Wilson's claims. The tested claims are the two finite maps of Proposition [fdip-00A0]: conjugation \(SU(2)\to SO(3)\) and the quotient \(2T\to A_4\), both with kernel \(\{1,-1\}\). The larger proposals in § [fdip-00A2] stay open. Three of the 4 Lie names do not occur in the cited Wilson paper, and the Hessian and \(SL(4,\mathbb R)\) claims are recorded there as interpretations. The absence of a construction is not a no-go theorem and not a physical identification.

Next questions. What remains can be stated as 4 questions. The physical environment map \(E\) is still unconstructed. The continuum comparison is still the one fixed Fourier mode of Proposition [fdip-004J]. The higher-dimensional area law, fermion reflection positivity and fermion transfer, and infinite-volume reconstruction were not proved. Whether continuous space comes back at large scales, without being supplied, is left to a separate plan; § 2 asks it and does not answer it. The enriched background groupoid and the geometric realization still do not supply a site, a stack, or a descent. Whether the context square organises the selectors remains open, and no stack is proved. Wilson's finite maps are tested, and the larger proposals remain open tests.