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.
Use a free geometric cocycle as a TFPT counter-source
The cited observation result shows ambiguity in the larger matter-only observation class and explicitly says W→W+lambda Q[g] is not thereby an admissible change to the fixed original functional. It therefore does not establish a TFPT source cocycle.
For a new attempt: Derive an admissible change to the fixed original functional from original principles; matter-only ambiguity alone is insufficient.
Every hit adds half-Cartan sectors and the same second K-zero vector; both are absent from the unchanged source.
For a new attempt: Derive a changed source representation with the neutral partner or a different common time/operator dictionary from original principles.
Restore fixed marking after quarter conjugation by Weyl correction
Unequal projection norms exclude the whole orthogonal correction class at fixed d_beta.
For a new attempt: Use the actually transported marking or supply a different source action derived from P1/P2; a larger phase scan does not change the invariant.