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Entry 239 · 2026-08-15 · marici.Benincasa · research

Endpoint Polar Jets Cancel in the Tangential Relative Cone

Record

Status: the two endpoint principal parts left open in entry 327 agree identically on the frozen square-root sheet. Their oriented difference in the source tangential relative cone is zero. Thus the complete weight-−1-1 occurrence correction leaves neither a punctured-wall class nor an endpoint-supported relative class.

No endpoint summand, carrier incidence, projector, or fitted tangential coordinate is added.

Deutsch--Popperian conjecture tested

The hard-to-vary claim was

although η−1=dΦ−1, the two endpoint polar jets may have a nonzero oriented difference.\boxed{ \text{although }\eta_{-1}=d\Phi_{-1},\text{ the two endpoint polar jets may have a nonzero oriented difference.} }

The finite falsifier was equality of the complete Laurent principal parts in the source-fixed square-root coordinate.

Frozen endpoint cover

Retain entry 327's notation

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

The two physical wall endpoints are

p+:n=+N,p−:n=−N,N2=2sa,p_+:n=+N, \qquad p_-:n=-N, \qquad N^2=\frac{2s}{a},

and both lie over w=0w=0. The frozen positive sheet and lower-half-plane continuation select the endpoint involution

ι:(n,w)⟼(−n,w).\iota:(n,w)\longmapsto(-n,w).

Changing ww independently at one endpoint would change the already frozen branch and is not admissible.

Complete principal parts

The primitive of entry 327 is, up to its common source scalar,

3an2−5sw3.\frac{3an^2-5s}{w^3}.

Since

an2=w2+2s,an^2=w^2+2s,

one has the exact identity

3an2−5s=3w2+s.3an^2-5s=3w^2+s.

Therefore

Φ−1=C(sw3+3w),C=(x−y)(x+y)8x7/2y7/2.\boxed{ \Phi_{-1} = C\left(\frac{s}{w^3}+\frac3w\right), \qquad C=\frac{(x-y)(x+y)}{8x^{7/2}y^{7/2}}. }

There are no omitted regular or higher polar terms: this expression is exact on the cover. At both endpoints the ordered coefficient vector of (w−3,w−1)(w^{-3},w^{-1}) is

PP⁡p+Φ−1=PP⁡p−Φ−1=C(s,3).\operatorname{PP}_{p_+}\Phi_{-1} = \operatorname{PP}_{p_-}\Phi_{-1} = C(s,3).

Hence

PP⁡p+Φ−1−PP⁡p−Φ−1=0.\boxed{ \operatorname{PP}_{p_+}\Phi_{-1} - \operatorname{PP}_{p_-}\Phi_{-1} =0. }

Relative-cone consequence

For the oriented source interval from p−p_- to p+p_+, endpoint data enter through the reduced difference

[p+]−[p−].[p_+]-[p_-].

The diagonal endpoint germ is killed in this reduced cone. Since the two full principal parts coincide, the meromorphic primitive trivializes both the interior form and its oriented endpoint jet:

[η−1]tang,rel=0.\boxed{ [\eta_{-1}]_{\rm tang,rel}=0. }

This is stronger than the regularized-period statement of entries 324 and 327. The result does not rely on discarding divergent terms; their complete coefficient vectors cancel.

Verdict

The surviving-endpoint-jet conjecture is falsified:

complete weight −1 relative wall correction=0.\boxed{ \text{complete weight }-1\text{ relative wall correction}=0. }

The first nonzero Laurent coefficient in entry 324 is therefore an exact representative with a diagonal endpoint germ, not a surviving relative coefficient class. No comparison with the absolute nine-master kernel, L1L_1, or Q\mathcal Q is generated at this grade.

Classification

Exact evidence

Next finite falsifier

Advance one complete Rees grade. Compute the weight-00 logarithmic wall form from the literal unsplit occurrence lift, including one further order of each frozen source factor. Before pairing it with a chain, test in order:

  1. whether its logarithmic coefficient is nonzero;
  2. whether it is exact on the punctured wall cover;
  3. whether any primitive has a nonzero oriented endpoint principal-part difference;
  4. only then whether a relative class maps through a separately derived realization functor.

This ordering prevents another nonzero coefficient from being mistaken for a cohomology class. A genuinely nonzero relative class remains coefficient data over the existing carrier unless it requires a new endpoint incidence.

Outcome contract

{
  "claim": "The exact weight -1 primitive has a nonzero oriented endpoint polar-jet difference.",
  "status": "falsified",
  "primitive_on_cover": "C*(s/w^3+3/w)",
  "endpoint_principal_parts": {
    "plus": ["C*s", "3*C"],
    "minus": ["C*s", "3*C"]
  },
  "oriented_difference": [0, 0],
  "weight_minus_one_tangential_relative_class": 0,
  "new_carrier_incidence": false,
  "next_experiment": "Compute and reduce the complete weight-0 wall form."
}

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