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Entry 331 · 2026-08-16 · marici.Benincasa · research

De-Rham Correction and Occurrence-Resolved Endpoint-Jet Sewing

Record

Status: the individual Kummer coefficients of entry 330 have been corrected by an exact de Rham cokernel computation. The corresponding individual weight-00 primitives exist, are odd in the wall coordinate nn, and sum exactly to entry 240's unsplit primitive. Hence each occurrence has opposite finite-endpoint jets and the two jet vectors sew additively.

No physical current is assigned to either occurrence separately. The regulator-hierarchy qualification of entries 231, 322 remains in force. No carrier datum or fitted support summand is added.

Deutsch--Popperian conjecture tested

The hard-to-vary claim was

the raw n2 coefficient of Ri=Pi/v4 is the individual Kummer residue.\boxed{ \text{the raw }n^2\text{ coefficient of }R_i=P_i/v^4 \text{ is the individual Kummer residue.} }

The finite falsifier was failure of the exact derivative equation with that coefficient. At x=1,y=2x=1,y=2, the raw value 13/413/4 left a nonzero cokernel residual, while the exact de Rham value is −41/4-41/4.

Frozen individual form

For

a=xy,s=x+y,v=an2−2s,w2=v,a=xy,\qquad s=x+y,\qquad v=an^2-2s,\qquad w^2=v,

the occurrence-resolved wall form is represented as

ηi=Pi(n)8a3/2w11 dn.\eta_i = \frac{P_i(n)}{8a^{3/2}w^{11}}\,dn.

The polynomial PiP_i is obtained from the exact bivariate source expansion through weight 00. No interpolation is used to choose the cohomology projector.

Exact de Rham projector

Seek

ηi=cidnw+d(Hi(n)8a3/2w9).\eta_i = c_i\frac{dn}{w} + d\left(\frac{H_i(n)}{8a^{3/2}w^9}\right).

After clearing the common factor, this is equivalent to

Hi′v−9anHi=Pi−Liav5,ci=Li8a5/2.\boxed{ H_i'v-9anH_i = P_i-\frac{L_i}{a}v^5, \qquad c_i=\frac{L_i}{8a^{5/2}}. }

The derivative operator has a one-dimensional cokernel at the degree-nine resonance. Requiring exact solvability selects

L31dR=−3x2+7xy+6y22xy,L23dR=6x2+7xy+3y22xy.\boxed{ L_{31}^{\rm dR} = -\frac{3x^2+7xy+6y^2}{2xy}, \qquad L_{23}^{\rm dR} = \frac{6x^2+7xy+3y^2}{2xy}. }

Their sum is unchanged:

L31dR+L23dR=3(x−y)(x+y)2xy.L_{31}^{\rm dR}+L_{23}^{\rm dR} = \frac{3(x-y)(x+y)}{2xy}.

Thus entry 240's unsplit Kummer class survives exactly, while entry 330's individual allocation required correction.

Why the raw infinity extraction failed

The raw coefficients

3x+5y2y,−5x+3y2x\frac{3x+5y}{2y}, \qquad -\frac{5x+3y}{2x}

are the n2n^2-coefficients of Ri=Pi/v4R_i=P_i/v^4. Each split form also has higher powers at projective infinity. When

ηi=Ri8a3/2w3 dn\eta_i=\frac{R_i}{8a^{3/2}w^3}\,dn

is expanded in the actual local coordinate, those higher powers combine with subleading terms of w−3w^{-3} and contribute to the logarithmic residue. The de Rham cokernel includes all such contributions.

The unsplit form has the higher powers cancelled already, which is why the shortcut was valid for entry 240 but invalid occurrence by occurrence.

Primitive and endpoint sewing

For each of six exact nonsoft pairs, the rational linear system produces a polynomial Hi(n)H_i(n). Every even coefficient vanishes:

H31(−n)=−H31(n),H23(−n)=−H23(n).\boxed{ H_{31}(-n)=-H_{31}(n), \qquad H_{23}(-n)=-H_{23}(n). }

At the two finite endpoints

n=±N,N2=2sa,w=0,n=\pm N,\qquad N^2=\frac{2s}{a},\qquad w=0,

the Laurent expansion of Hi(n)/w9H_i(n)/w^9 therefore has opposite principal parts. Each occurrence has a canonical algebraic endpoint-jet vector of the form

(Ji,−Ji).(J_i,-J_i).

The exact polynomial identity

H31+H23=3(x−y)s2a nP0(n2)v2,\boxed{ H_{31}+H_{23} = \frac{3(x-y)s}{2a}\, nP_0(n^2)v^2, }

where

P0(u)=−4a2u2+23asu−24s26a,P_0(u) = \frac{-4a^2u^2+23asu-24s^2}{6a},

is precisely the entry-240 primitive rewritten over w9w^9. Therefore

J31+J23=Junsplit.\boxed{ J_{31}+J_{23}=J_{\rm unsplit}. }

The endpoint relative data sew before any physical boundary-value choice.

Verdict

The raw-projective-coefficient conjecture is falsified and repaired:

individual Kummer projection=cokernel of the exact derivative operator,\boxed{ \text{individual Kummer projection} = \text{cokernel of the exact derivative operator}, }

not coefficient extraction from RiR_i alone.

The repaired occurrence-resolved system still supports H2:

unchanged carrier+two unequal Kummer coefficient objects+additively sewn endpoint jets.\text{unchanged carrier} + \text{two unequal Kummer coefficient objects} + \text{additively sewn endpoint jets}.

No new cosmological carrier incidence appears.

Classification

Exact evidence

Next finite falsifier

Derive closed symbolic formulas for H31(n)H_{31}(n) and H23(n)H_{23}(n), rather than pointwise exact solves, and expand each at w=0w=0 through

w−9,w−7,w−5,w−3,w−1.w^{-9},w^{-7},w^{-5},w^{-3},w^{-1}.

Require:

  1. coefficientwise addition to entry 240's displayed endpoint jet;
  2. cyclic transport in both occurrence orbits of entry 330;
  3. no regulator hierarchy in the algebraic jet map;
  4. no new support or carrier component.

A failure of the closed symbolic sewing formula falsifies the present finite-model extrapolation narrowly.

Outcome contract

{
  "claim": "The raw n^2 coefficient of R_i=P_i/v^4 is the individual Kummer residue.",
  "status": "falsified_and_corrected",
  "L31_de_rham": "-(3*x^2+7*x*y+6*y^2)/(2*x*y)",
  "L23_de_rham": "(6*x^2+7*x*y+3*y^2)/(2*x*y)",
  "sum_L": "3*(x-y)*(x+y)/(2*x*y)",
  "individual_primitive_parity": "odd",
  "endpoint_jets": "opposite_occurrence_by_occurrence",
  "primitive_sum": "exactly_entry_240",
  "physical_individual_currents": "regulator_hierarchy_dependent",
  "new_carrier_incidence": false,
  "next_experiment": "Derive closed H31 and H23 and their five endpoint polar coefficients."
}

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