Follow the published construction into its registered claims, then explore reviewed research questions, attempts and the connections that remain open.
Seam, origin and declared inputs
The published foundation in this area
25 authored claim references lead into the original ledger and paper sections. This source record remains available even where no separate reviewed research packet is attached.
TFPT starts from the oriented seam normalization P1 (c3=1/(8π)) and the marked five-slot carrier P2. Integer anchors and later compiler readouts connect these inputs, but do not derive their physical origin or selection.
Starting structure in the Atlas orientation
P1 declares c3=1/(8π); P2 declares five carrier slots with a 3+2 marking. The (1,1,2) anchor organizes internal numerical relations.
Which connection is sought
The open work is a non-circular source for these inputs, the physical seam, and derivations of their markings and readout rules.
How it connects
The declared seeds feed E8, clock, flavor, α, and scale readouts. Shared seeds make those outputs correlated.
For a new attempt: Firstderiveactualchargedlocalalgebra/fielddictionaryfromoriginaloperations;thenapplyKMS/modulartransport.Donotuseglobalrotationonfixedintervalaslocalmodulartime.
For a new attempt: ConstructoriginallyjustifiedchangedCartan/statistics/netmapwithchargedfieldcarrier,fullwords,timeandprimitivewindingcomparison.Nospectral/KMSclaimasasubstitute.
Derive existing parity-Gauss rule only from original P1 definitions
Forward source comparison identifies a concrete insertion/localization definition gap. The seed already takes the local net as input; no inverse selection of the gauge net or full P1 compatibility of both models is proved.
For a new attempt: Build no further extension. A later decision needs the originally defined local insertion/sector map with Padm/Gx, state, time, reflection and primitive winding identification. State this gap and stop.
The specific proof steps are audited; generic bound0 is refuted and replaced by correct conditional hypotheses. The source inverse still needs an actual defined local reconstruction.
For a new attempt: Continue only with a precise source map, complete correlators or newly proved symbol/domain bounds. A freely chosen helper model does not replace these conditions.
This inverse is analytically settled; do not repeat Hamiltonian search when complete G is supplied.
For a new attempt: For source selection supply the actual original graph kernel, fiber comparison and normal length; G generated from a guessed B is not a provenance derivation.
Do not repeat homogeneous GKSL time search for the fixed M4 channel
The all-branch proof also excludes every positive integer power.
For a new attempt: Time-dependent execution or a larger justified source is a different comparison class, not a repair of the same homogeneous M4 generator.