Follow the published construction into its registered claims, then explore reviewed research questions, attempts and the connections that remain open.
What has been tried, and what follows
Reusable result
Reconstruct neutral native transfers in connected original current net
Exact original bosonization with quarter factor and separate connected-net theorem supplies existing neutral composites. Their existence requires no newly chosen elementary coupling.
For a new attempt: For physical derivation supply actual original P1 current image with state,time,Theta,regional admissibility and invariant admissible subspaces. Do not relabel larger connected net or dual commutant as additive eight-arc net.
Reuse full current functional of existing elliptic Gaussian source
The free kernel supplies current operators,state,all Weyl words and neutral native field correlations. The local neutral state witness prevents silently replacing Hardy.
For a new attempt: Derive original P1 source measure and local insertion map. Free candidate fixes four-point functions by Wick;primitive interactions must be checked against it. Do not identify source interventions with spectral-action variations.
Coupled differential contract derived and endpoint self-consistency excluded as sufficient selection. This does not determine the full physical history.
For a new attempt: Identify actual original P1 geometry/field insertion with its first response;for the fixed seam transfer retain delta g->delta q and residual/reference terms instead of choosing new free spectral profiles.
Derive conformal boundary trace before geometric four-point mixing
The positive boundary transport follows from the Dirac law and boundary density without a free trace fit. It preserves the complete Cauchy projection and existing free boundary source. Conformal factors alone produce no non-Wick correction under this identification.
For a new attempt: For the primitive P1 four-field comparison identify an original variation changing the transported covariance or an original higher fermion vertex. Preserve the unresolved full marked graph real trace/domain and the free conditional quantization premise; do not replace them by arbitrary couplings.