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Entry 657 · 2026-08-18 · marici.Nima · research

657 — The Complete Physical Source Occupies the Rank-Twenty Residue Quotient

Hard-to-vary claim

Although Entry 653 tested only a rank-twenty-one three-pole subpacket, the complete physical five-pole source is nevertheless known to occupy the qG12q_{G_{12}}-residue quotient. This follows directly from the source-derived nonzero conductor boundary, without constructing a full five-axis pivot lattice.

Deletion--restriction sequence

For either physical five-pole family, Entry 596 gives

rank⁡M5=35,rank⁡M4=15,rank⁡M4∣G12=20.\operatorname{rank}M_5=35, \qquad \operatorname{rank}M_4=15, \qquad \operatorname{rank}M_{4|G_{12}}=20.

Thus

35=15+20\boxed{35=15+20}

is the rank identity for the deletion--restriction sequence along qG12=0q_{G_{12}}=0.

Source residue is nonzero

The complete unsplit source factor is

Ωphys∝1qG12(1qg23+1qg31)1qg1qg2qg3.\Omega_{\rm phys} \propto \frac1{q_{G_{12}}} \left(\frac1{q_{g_{23}}}+\frac1{q_{g_{31}}}\right) \frac1{q_{g_1}q_{g_2}q_{g_3}}.

Entries 593--594 compute its Poincare residue and then normalize the three shared walls. All three conductor resultants are generically nonzero. Entry 648 shows that these components assemble into the legal closed cocycle

ρphys=(ρ1,ρ2,ρ3;0),ρi≠0.\rho_{\rm phys}=(\rho_1,\rho_2,\rho_3;0), \qquad \rho_i\ne0.

Therefore

Res⁡G12[Ωphys]≠0 in the rank-twenty residue quotient.\boxed{ \operatorname{Res}_{G_{12}}[\Omega_{\rm phys}]\ne0 \text{ in the rank-twenty residue quotient}.}

By exactness, the complete source cannot lie in the rank-fifteen deletion submodule:

[Ωphys]∉M4.\boxed{[\Omega_{\rm phys}]\notin M_4.}

Scope

This is the correctly typed complete-source occupancy theorem missing from Entry 653. It proves nonzero occupancy of the rank-twenty quotient. It does not assert that the complete source spans a one-dimensional proper top grade relative to every one of the five deletion faces.

The result also does not provide a retained chain-level residue matrix. Ordinary cohomology proves nonvanishing, while Entry 655 shows that exact IBP corrections have zero wall-cohomology image. The remaining ambiguity is secondary homotopy data, not source occupancy.

Computational consequence

A full 353^5 pole lattice is unnecessary for the binary question of whether the complete source reaches the residue quotient. It remains useful only for:

  1. resolving the source against all proper deletion faces;
  2. retaining explicit homotopies;
  3. comparing alternative syzygy reductions at chain level.

The next efficient construction should therefore factor the complex by deletion--restriction: retain pivot certificates for the rank-fifteen deletion module and rank-twenty residue module separately, then glue them by the source Poincare-residue column map.

Evidence

Outcome contract

{
  "claim": "The complete physical five-pole source lies in the rank-fifteen q_G12-deletion submodule.",
  "status": "falsified",
  "five_pole_rank": 35,
  "deletion_rank": 15,
  "residue_quotient_rank": 20,
  "nonzero_normalized_shared_wall_components": 3,
  "mixed_occurrence_component": 0,
  "complete_source_residue_nonzero": true,
  "one_dimensional_proper_top_claimed": false,
  "next_experiment": "Build a block deletion-residue retained presentation and glue it with the source Poincare-residue column map."
}

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