Established in scope
Explicit graded inverse extracts unintegrated body weight from source coefficients
In the question: Recursion, hypergraphs and mirroring at the original joint source
Elementary finite constructive inverse,no novelty claim or numerical primitive boson distribution. Top probe needs actual original insertion/contact map and full admissibility;gauge neutrality does not prove Pgap reduction. Nonmultiplicative selectors give body of whole kernel,not automatically unselected exp(-SB). Retain ghost/odd directions and original determinant line. No measure or normalization selected;source values must actually be available. SOURCEINV20261104: Physical application attempted but not executed. Conditional coherent boundary symbol is not identified with full bulk Grassmann density; body multiplier cannot be pulled through the whole selector without its commutator term. Invisible ambient extensions do not prove physical nonuniqueness, and uncomputed source values do not establish a need for another measure or axiom. No new physical Sadm/Htrpos/spectrum.
Read the exact result, assumptions and evidence
Result
Actual finite ordered Grassmann pairing gives L[f theta^(Ic)]=sigma(I) int f wI and reconstructs every coefficient density. Saturated tau isolates w0 without Pfaffian inversion,also at zero Pfaffian and with higher vertices. Finite nilpotent log gives action on nonzero body branch. Reynolds averaging in original invariant JOINT pairing separates invariant densities without elementary charged observables. Exact controls:all8 even coefficients,log roundtrip,invariant pairing rank6 det-1,zero partition with extracted body1.
Required assumptions
- Do not identify source types
Observable algebra, OS reflection, state, collar operator, time evolution, carrier connection, family holonomy, and readout are distinct data until an original map relates them.
- Actual finite graded source pairing with original orientation
Supplied original finite Grassmann coordinates,original boson/rest integration and complete ordered source values with correct contacts. Inverse probes apply only in actual admissible test space or established invariant quotient;parity does not imply admissibility.
Original evidence
- BEREZIN-INVERSE.txt lines 1–180
Source checked at this snapshot
Original location and fingerprint
experiments/theory-contracts/recursive-mirrored-source-20261103/BEREZIN-INVERSE.txt
8715fb914a5621c894463133820bcc84374fd6ee397cb6e9593cd9f13bce05a4
- BEREZIN-INVERSE.txt lines 181–208
Source checked at this snapshot
Original location and fingerprint
experiments/theory-contracts/recursive-mirrored-source-20261103/BEREZIN-INVERSE.txt
8715fb914a5621c894463133820bcc84374fd6ee397cb6e9593cd9f13bce05a4
- berezin-inverse-results.json lines 1–20
Source checked at this snapshot
Original location and fingerprint
experiments/theory-contracts/recursive-mirrored-source-20261103/berezin-inverse-results.json
aaf2cc13c9ea80eedaf881abd96e9b28b12497080c346d57bdf39db2071a6d72
- SOURCE-INVERSE-APPLICATION-I.txt lines 1–58
Source checked at this snapshot
Original location and fingerprint
experiments/theory-contracts/recursive-mirrored-source-20261103/SOURCE-INVERSE-APPLICATION-I.txt
0cae62189413db422df22abe26cfe5f0053f17c2cd2ee2cd5a68c26ccea05113
finding:rec20261103c-graded-source-inverse-extracts-unintegrated-body