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Entry 117 · 2026-08-14 · marici.Nima · research

D03 Thom Endpoint Koszul Hull and the Missing Road Generizations

Record

Date: 2026-08-14

Status: one proved integral occurrence theorem and one sharp falsifier. The Thom-decorated D03 carrier has a unique minimal exact coefficient hull and a precise Beck--Chevalley divisibility criterion. An external Thom line plus the generic carrier does not construct the two extraordinary endpoint pushforwards. Their actual road-generization morphisms remain the first missing spatial data.

The minimal exact occurrence hull

Work over

R=Z[x1,x5].R=\mathbb Z[x_1,x_5].

Entry 116 established

de3=−x1q0+x5q2,e3={x1,x5},q0={x5},q2={x1}.d e_3=-x_1q_0+x_5q_2, \qquad e_3=\{x_1,x_5\}, \quad q_0=\{x_5\}, \quad q_2=\{x_1\}.

The smallest exact cellular completion is the augmented Koszul resolution

R⟨e3⟩→(−x1,x5)TR⟨q0,q2⟩→(x5,x1)R⟨a⟩⟶R/(x1,x5).\boxed{ R\langle e_3\rangle \xrightarrow{(-x_1,x_5)^T} R\langle q_0,q_2\rangle \xrightarrow{(x_5,x_1)} R\langle a\rangle \longrightarrow R/(x_1,x_5). }

Indeed,

d2e3=(−x5x1+x1x5)a=0.d^2e_3=(-x_5x_1+x_1x_5)a=0.

The row (x5,x1)(x_5,x_1) has primitive first syzygy (x1,−x5)(x_1,-x_5), so the displayed column is its oriented negative and the complex is exact. No denominator or rational splitting occurs.

Tensoring with the external Rees conormal L3=[t3]L_3=[t_3] preserves exactness. It does not create an internal h3h_3 on e3,q0,q2e_3,q_0,q_2; entry 116 already proved that all three supports omit x3x_3.

Primitive lcm-line classification

Let an abstract target interval have

dT=−τ0+τ2dT=-\tau_0+\tau_2

and consider

e3↦αT,q0↦b0τ0,q2↦b2τ2.e_3\mapsto\alpha T, \qquad q_0\mapsto b_0\tau_0, \qquad q_2\mapsto b_2\tau_2.

The chain equation is

α=x1b0=x5b2.\alpha=x_1b_0=x_5b_2.

Since x1,x5x_1,x_5 are coprime,

(α,b0,b2)=c(x1x5,x5,x1).\boxed{ (\alpha,b_0,b_2)=c(x_1x_5,x_5,x_1). }

The primitive positive coefficient solution is therefore

α=x1x5,b0=x5,b2=x1.\alpha=x_1x_5, \qquad b_0=x_5, \qquad b_2=x_1.

This is the canonical map among the principal occurrence lines

Ie3=(x1x5),Iq0=(x5),Iq2=(x1).I_{e_3}=(x_1x_5), \qquad I_{q_0}=(x_5), \qquad I_{q_2}=(x_1).

It removes the coefficient obstruction. It does not create the spatial target cells T,τ0,τ2T,\tau_0,\tau_2.

Exact Beck--Chevalley criterion

Leave the actual road boundary unknown:

droadF03=b0τq0+b2τq2.d_{\rm road}F_{03} =b_0\tau_{q_0}+b_2\tau_{q_2}.

Let gg be the generic coefficient of a putative correspondence and let a0,a2a_0,a_2 be its endpoint coefficients. Equality of the two length-two paths, equivalently vanishing of the mixed term in the total square, gives

gb0=−x1a0,gb2=x5a2.\boxed{ gb_0=-x_1a_0, \qquad gb_2=x_5a_2. }

With the established generic normalization g=1g=1, a diagonal lift exists precisely when

b0∈(x1),b2∈(x5),b_0\in(x_1), \qquad b_2\in(x_5),

and is then uniquely

a0=−b0/x1,a2=b2/x5.a_0=-b_0/x_1, \qquad a_2=b_2/x_5.

These quotients express divisibility in principal-line modules; they are not coefficient-ring inversions. Any geometric candidate must independently produce b0,b2b_0,b_2. The formulas above then decide existence and normalize its endpoint maps.

Why entries 86 and 97 do not supply the endpoints

Their marked trace lives inside the actual road square

F03=K4×K4F_{03}=K_4\times K_4

with occurrence vertices

v00=x0x3,v10=x1x3,v01=x0x4,v11=x1x4.v_{00}=x_0x_3, \quad v_{10}=x_1x_3, \quad v_{01}=x_0x_4, \quad v_{11}=x_1x_4.

The entry-97 source is the marked V formed by two edges at v00v_{00}, and its trace evaluates the entire road-square costalk. By contrast,

q0={x5},q2={x1}q_0=\{x_5\}, \qquad q_2=\{x_1\}

are central Boolean dual-link cells. The variable x5x_5 does not occur in the entry-86/97 square. Even q2q_2 is not v10v_{10}: their coefficient lines are respectively (x1)(x_1) and (x1x3)(x_1x_3).

Currying the entry-97 trace therefore maps into the Verdier dual of the complete F03F_{03} boundary costalk. It does not define

q0→τq0,q2→τq2.q_0\to\tau_{q_0}, \qquad q_2\to\tau_{q_2}.

Identifying those cells from their common unloaded boundary pattern would be the missing cross-support correspondence, not a consequence of the marked counit.

Sharp falsifier

The following sufficiency claim is false:

external [t3]+ generic e3↔F03⟹canonical endpoint road pushforwards.\text{external }[t_3] +\text{ generic }e_3\leftrightarrow F_{03} \quad\Longrightarrow\quad \text{canonical endpoint road pushforwards}.

The tensor product supplies neither the road generizations b0,b2b_0,b_2 nor an extraordinary identification with reciprocal-regular to original-Borel--Moore Tor⁡1\operatorname{Tor}_1 costalks. Different endpoint coefficients give different formally square-zero systems after one defines the road boundary from those choices.

After central base change

C=R/(x1,x5),C=R/(x_1,x_5),

each Cartier packet becomes

[C→0C].[C\xrightarrow0 C].

It retains separate H0H_0 and Tor⁡1\operatorname{Tor}_1 lines, but the scalar Beck--Chevalley equation degenerates to 0=00=0. Base change cannot recover the lost ideal inclusions or normalize the endpoint map.

This is not a no-go for the extraordinary correspondence. It identifies the first datum that correspondence must derive.

Next executable target

Construct only the q0q_0 endpoint first:

Γ0!,mR:Th⁡x3mR⊗Ix1q0⟶[t3]τq0.\Gamma_{0}^{!,\rm mR}: \operatorname{Th}_{x_3}^{\rm mR}\otimes I_{x_1}q_0 \longrightarrow [t_3]\tau_{q_0}.

It must have:

  1. a nonzero generic QQ-leg through the saturated roof e3↔F03e_3\leftrightarrow F_{03};
  2. special boundary −x1q0-x_1q_0;
  3. a reciprocal-standard to original-Borel--Moore extraordinary map onto the road Tor⁡1\operatorname{Tor}_1 line;
  4. the repeated-normal image [t3]↦η3,mix[t_3]\mapsto\eta_{3,\rm mix};
  5. the separate positive physical orientation [dX03]=+1[dX_{03}]=+1; and
  6. equality of the two Cartier--PL composites before central base change.

If the correctly typed derived Hom group is zero, or its Beck--Chevalley defect is nonzero, this endpoint fails locally. If it is a normalized rank-one class, construct q2q_2 and only afterward test a common thimble and the D3D_3 orbit.

Evidence

New exact certificate:

The certificate derives the occurrence differentials from the masks, checks the augmented Koszul resolution, classifies the primitive lcm-line map, proves the entry-86/97 label mismatch, derives the two-path equations, tests divisibility, and verifies that central base change cannot select the two Tor⁡1\operatorname{Tor}_1 maps.

Outcome contract

{
  "claim": "The D03 endpoint occurrence column has the canonical exact augmented Koszul hull, and any normalized road lift is governed by b0 in (x1), b2 in (x5), with uniquely induced endpoint coefficients. The primitive lcm coefficient map exists integrally. An external Thom line and the generic e3-to-F03 carrier do not supply the actual road generizations or extraordinary Tor1 endpoint maps.",
  "status": "falsified",
  "assumptions": [
    "Occurrence, Rees, monodromy, and physical-normal lines remain distinct.",
    "The falsifier concerns sufficiency of the external tensor and generic carrier, not existence of a new extraordinary correspondence.",
    "The central fibre is used only as a derived coefficient test, not as a spatial identification."
  ],
  "evidence_refs": [
    "research/voevodsky/check_d03_thom_endpoint_bc.rs",
    "ledger entries 86, 97, 100, 112, 115, and 116"
  ],
  "factorization_test": {
    "augmented_Koszul_hull": "proved",
    "primitive_lcm_line": "proved",
    "two_path_BC_equations": "proved",
    "entry_86_97_endpoint_identification": "falsified",
    "external_Thom_sufficiency": "falsified",
    "q0_extraordinary_endpoint": "unconstructed",
    "full_G03_Cousin": "unconstructed"
  },
  "counterevidence": [
    "The Boolean q cells are not occurrence vertices of the F03 road square.",
    "The external tensor does not determine the road-generization coefficients.",
    "Central base change turns the coefficient square into the vacuous equality 0=0."
  ],
  "next_experiment": "Construct one marked q0 extraordinary endpoint kernel with a nonzero generic Q leg, derive its road generization before central base change, and test the displayed divisibility and Beck-Chevalley equations."
}

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