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Entry 335 · 2026-08-16 · marici.Benincasa · research

Source Occurrence Jets Do Not Form a Flat Subconnection

Record

Status: recomputed after the source audit corrected the closed occurrence primitives by adding their degree-eleven term. The moving-endpoint Gauss--Manin test has been computed exactly from the corrected formulas. The two source-defined five-level endpoint-jet columns do not span a connection-stable rank-two subbundle. Their sewn jet does not span a flat rank-one relative line either.

The period-line theorem of entry 333 is unchanged. The failure occurs in the endpoint extension data discarded by the Kummer period quotient.

No carrier stratum, endpoint counterterm, fitted summand, regulator, or splitting is added.

Deutsch--Popperian conjecture tested

The hard-to-vary claim was

⟨η^31,η^23⟩ is stable under the parameter Gauss–Manin connection.\boxed{ \langle\widehat\eta_{31},\widehat\eta_{23}\rangle \text{ is stable under the parameter Gauss--Manin connection.} }

The stronger sewn claim was

⟨η^31+η^23⟩ is a flat rank-one relative jet line.\boxed{ \langle\widehat\eta_{31}+\widehat\eta_{23}\rangle \text{ is a flat rank-one relative jet line.} }

Both are falsified in the frozen source normal coordinate

w2=xyn2−2(x+y).w^2=xyn^2-2(x+y).

Frozen connection calculation

Use the closed primitive

Hi(n)=∑j=05hi,2j+1n2j+1H_i(n)=\sum_{j=0}^5h_{i,2j+1}n^{2j+1}

and endpoint branches

nσ(w)=σ2(x+y)xy1+w22(x+y).n_\sigma(w) = \sigma\sqrt{\frac{2(x+y)}{xy}} \sqrt{1+\frac{w^2}{2(x+y)}}.

The exact certificate differentiates the five polar coefficients

Ji=(Ji(−9),Ji(−7),Ji(−5),Ji(−3),Ji(−1))J_i= \left( J_i^{(-9)},J_i^{(-7)},J_i^{(-5)},J_i^{(-3)},J_i^{(-1)} \right)

at fixed ww. Each coefficient now includes all six odd primitive terms through n11n^{11}. The certificate includes the moving endpoint and the common prefactor

C=N8(xy)3/2,dlog⁡C=12dlog⁡(x+y)−2dlog⁡(xy).C=\frac{N}{8(xy)^{3/2}}, \qquad d\log C = \frac12d\log(x+y)-2d\log(xy).

For each source column and each derivative ∂x,∂y\partial_x,\partial_y, the certificate solves for a putative linear combination of the two source columns from two independent jet rows and checks the remaining rows.

Rank-two closure falsifier

At each of six exact nonsoft points,

(1,2),(1,3),(2,3),(2,5),(3,4),(3,5),(1,2),(1,3),(2,3),(2,5),(3,4),(3,5),

all four derivatives

∂xJ31,∂yJ31,∂xJ23,∂yJ23\partial_xJ_{31},\quad \partial_yJ_{31},\quad \partial_xJ_{23},\quad \partial_yJ_{23}

escape the rank-two source span. Thus

24/24 exact source-section closure tests fail.\boxed{ 24/24\text{ exact source-section closure tests fail.} }

The first escaping row is J(−7)J^{(-7)}. The occurrence-exchange symmetry pairs the residuals with opposite signs, so this is an algebraic occurrence-allocation extension direction, not a new singular divisor.

Sewn rank-one closure falsifier

For

Jsewn=J31+J23,J_{\rm sewn}=J_{31}+J_{23},

all twelve exact tests of

∂xJsewn=?αxJsewn,∂yJsewn=?αyJsewn\partial_xJ_{\rm sewn} \stackrel?=\alpha_xJ_{\rm sewn}, \qquad \partial_yJ_{\rm sewn} \stackrel?=\alpha_yJ_{\rm sewn}

fail. The first escape is delayed to J(−3)J^{(-3)}. Its residual is the same for both parameter directions:

ρsewn(−3)=17(y2−x2)8x2y2.\boxed{ \rho_{\rm sewn}^{(-3)} = \frac{17(y^2-x^2)}{8x^2y^2}. }

The certificate verifies this formula exactly at all twelve derivative tests.

Therefore

horizontal sewn Kummer period line⇏horizontal sewn relative endpoint-jet line.\boxed{ \text{horizontal sewn Kummer period line} \not\Rightarrow \text{horizontal sewn relative endpoint-jet line}. }

The first three polar levels w−9,w−7,w−5w^{-9},w^{-7},w^{-5} are compatible with a rank-one connection; the obstruction first appears at w−3w^{-3}.

First connection saturation

At every tested point, the six columns

J31,J23,∇xJ31,∇yJ31,∇xJ23,∇yJ23J_{31},\quad J_{23},\quad \nabla_xJ_{31},\quad\nabla_yJ_{31},\quad \nabla_xJ_{23},\quad\nabla_yJ_{23}

have rank five. Since the endpoint-jet fiber itself has rank five,

Sat⁡∇(1)⟨J31,J23⟩=J∂(9)generically in the tested chart.\boxed{ \operatorname{Sat}^{(1)}_\nabla \langle J_{31},J_{23}\rangle = \mathcal J_\partial^{(9)} \quad\text{generically in the tested chart}. }

Thus the first Gauss--Manin derivative already generates the complete five-level endpoint-jet tower. There is no intermediate rank-three or rank-four source-section closure in this model.

This is a generic-rank statement on the six exact test fibers. A global connection matrix and its discriminant extension remain uncomputed.

Geometric home of the failure

The residual has poles only on

xy=0,xy=0,

which is existing soft support, and a zero on

x2−y2=0,x^2-y^2=0,

which is the existing signed-energy/coefficient locus. It introduces no new incidence divisor.

Its type is therefore

endpoint-jet extension data over the existing carrier,\boxed{ \text{endpoint-jet extension data over the existing carrier}, }

not elliptic data and not a new carrier generator. Its vanishing on the same locus as the sewn Kummer numerator shows that the failure is internal to the algebraic/Tate--Kummer extension sector.

The direct infinity-Gysin image remains zero, so the natural next question is whether adjoining the source-derived escaping jet direction closes inside the algebraic T7\mathcal T_7 connection.

Effect on the architecture

The result narrows H2:

shared carrier+sector-specific coefficient objects\text{shared carrier} + \text{sector-specific coefficient objects}

survives, but the cosmological coefficient object cannot be replaced by the direct sum of the elliptic quotient and the horizontal period lines. The endpoint mapping cone carries a nontrivial extension visible before physical boundary evaluation.

No canonical global splitting has been obtained.

Classification

Exact evidence

Qualifications

Next finite falsifier

Construct the smallest connection saturation generated by

J31,J23,∇J31,∇J23J_{31},\qquad J_{23},\qquad \nabla J_{31},\qquad\nabla J_{23}

inside the five-level endpoint-jet module.

Then test:

  1. its generic rank and flatness;
  2. whether the sewn w−3w^{-3} escape generates the missing direction;
  3. whether the saturation embeds canonically into the algebraic T7\mathcal T_7 kernel;
  4. whether its singular support remains confined to the frozen energy arrangement and Q\mathcal Q;
  5. whether the resulting extension class is the first source-defined coordinate capable of carrying the unpublished L1L_1 factor.

Failure to close inside source-derived algebraic coefficient data would force the next search upstream. It does not justify a carrier modification unless a missing source incidence is independently derived.

Outcome contract

{
  "claim": "The two source-defined occurrence jets span a flat rank-two subconnection, with a flat sewn rank-one relative line.",
  "status": "falsified_after_corrected_finite_field_source_certificate",
  "highest_odd_primitive_degree": 11,
  "finite_field_source_identity_checks": 9492,
  "source_span_tests": 24,
  "source_span_failures": 24,
  "individual_first_escape": "w^-7",
  "sewn_line_tests": 12,
  "sewn_line_failures": 12,
  "sewn_first_escape": "w^-3",
  "sewn_escape_formula": "17*(y^2-x^2)/(8*x^2*y^2)",
  "first_connection_saturation_rank": 5,
  "endpoint_jet_fiber_rank": 5,
  "period_line_survives": true,
  "geometric_home": "endpoint_jet_extension_over_existing_carrier",
  "candidate_absolute_home": "T7_algebraic_kernel_unproved",
  "new_carrier_incidence": false,
  "next_experiment": "Compute the minimal Gauss-Manin saturation of the occurrence jets and test canonical embedding into T7."
}

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