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Entry 240 · 2026-08-15 · marici.Benincasa · research

Weight-Zero Produces the First Genuine Relative Wall Class

Record

Status: the complete unsplit occurrence lift has a generic nonzero weight-00 logarithmic wall form. Unlike the weight-−1-1 form, it is not meromorphically exact. Its punctured-wall class is a rank-one Kummer class generated by dn/wdn/w, accompanied in the tangential relative realization by an opposite endpoint polar jet from an exact primitive.

This is the first genuine full-occurrence relative wall class in the tested grade sequence. It remains coefficient data over the frozen exceptional carrier and has zero direct infinity-Gysin image.

No carrier cell, endpoint summand, projector, or normalization is added.

Deutsch--Popperian conjecture tested

The hard-to-vary claim was

the complete weight 0 wall form is either zero or exact in the same sense as weight −1.\boxed{ \text{the complete weight }0\text{ wall form is either zero or exact in the same sense as weight }-1. }

The finite falsifier was a nonzero logarithmic residue at the two points at infinity of the frozen wall cover.

Frozen additional expansion layer

Retain the weighted chart and all source normalizations of entries 234--239. The new exact coefficients are

k3=−4n[−n2xy2+r3xy+r3y2+r2x2−r2xy−2r2y2−2rxy−ry2−x2−xy],\begin{aligned} k_3={}&-4n\bigl[ -n^2xy^2+r^3xy+r^3y^2+r^2x^2-r^2xy-2r^2y^2\\ &\hspace{38mm}-2rxy-ry^2-x^2-xy \bigr], \end{aligned}

ℓ3=−8n(x+y)(ry+x),\ell_3=-8n(x+y)(ry+x),

and

d3=n28r5x2y2[2n2r3xy−2n2r2xy+2n2rxy−2n2xy−r4x+r4y+2r3x+r3y−r2x−r2y].d_3= \frac{n^2}{8r^5x^2y^2} \left[ 2n^2r^3xy-2n^2r^2xy+2n^2rxy-2n^2xy -r^4x+r^4y+2r^3x+r^3y-r^2x-r^2y \right].

These are respectively the τ9\tau^9, τ7\tau^7, and relative τ3\tau^3 coefficients of KK, K1srcK_1^{\rm src}, and τ3Dlow\tau^3D_{\rm low}.

Exact logarithmic residue

Let

a=xy,s=x+y,u=n2,v=au−2s,a=xy, \qquad s=x+y, \qquad u=n^2, \qquad v=au-2s,

and retain

k00=4av.k_{00}=4av.

Reducing the weight-00 poles through order r−5r^{-5} gives

k003/2Res⁡r=0F0=3u(x−y)s(a2u2−7asu+5s2)2av2.\boxed{ k_{00}^{3/2}\operatorname{Res}_{r=0}F_0 = \frac{ 3u(x-y)s \left(a^2u^2-7asu+5s^2\right) }{2av^2}. }

This is even under n↦−nn\mapsto-n and generically nonzero. It vanishes on the symmetric locus x=yx=y, at n=0n=0, and on the proper roots of the displayed quadratic in uu, apart from excluded singular support.

On the physical branch,

Res⁡r=0F0=3(x−y)s16a5/2u(a2u2−7asu+5s2)v7/2.\operatorname{Res}_{r=0}F_0 = \frac{3(x-y)s}{16a^{5/2}} \frac{u(a^2u^2-7asu+5s^2)}{v^{7/2}}.

Meromorphic cohomology reduction

Compactify the already frozen wall cover

W:w2=v=an2−2s.W:\qquad w^2=v=an^2-2s.

Define

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

Exact differentiation gives

u(a2u2−7asu+5s2)w7 dn=1adnw+d(nP(u)w5).\boxed{ \frac{u(a^2u^2-7asu+5s^2)}{w^7}\,dn = \frac1a\frac{dn}{w} + d\left(\frac{nP(u)}{w^5}\right). }

The equality was checked after clearing denominators by the polynomial identity

(P+2uP′)v−5auP=u(a2u2−7asu+5s2)−1av3.\begin{aligned} &\left(P+2uP'\right)v-5auP\\ &\qquad= u(a^2u^2-7asu+5s^2)-\frac1a v^3. \end{aligned}

Therefore the surviving punctured-wall class is

[η0]=3(x−y)(x+y)16(xy)7/2[dnw].\boxed{ [\eta_0] = \frac{3(x-y)(x+y)}{16(xy)^{7/2}} \left[\frac{dn}{w}\right]. }

Finite falsifier at infinity

The compactified quadratic cover has two points at infinity, distinguished by

w∼σa n,σ=±1.w\sim\sigma\sqrt a\,n, \qquad \sigma=\pm1.

The core wall form has asymptotic behavior

u(a2u2−7asu+5s2)w7 dn∼σa−3/2dnn.\frac{u(a^2u^2-7asu+5s^2)}{w^7}\,dn \sim \sigma a^{-3/2}\frac{dn}{n}.

Thus its two residues are opposite and nonzero. Equivalently, dn/wdn/w has the standard two-puncture Kummer class. No meromorphic primitive can remove this term.

Hence

[η0]≠0\boxed{ [\eta_0]\ne0 }

at generic x≠yx\ne y.

These infinity points belong to the projective completion of the existing exceptional wall. They are not the anticanonical infinity divisor D∞D_\infty of the residue surface. Entry 325's direct elliptic Gysin vanishing is therefore unchanged.

Endpoint relative data

At the two finite branch endpoints w=0w=0, the exact primitive has opposite principal parts because n↦−nn\mapsto-n while ww remains fixed. Writing N2=2s/aN^2=2s/a,

nP(u)w5∼±Na[s2w5+17s12w3−1332w].\frac{nP(u)}{w^5} \sim \pm\frac Na \left[ \frac{s^2}{w^5} +\frac{17s}{12w^3} -\frac{13}{32w} \right].

Thus the correctly typed tangential relative object contains:

  1. the nonzero interior Kummer class [dn/w][dn/w];
  2. an occurrence-resolved opposite endpoint polar jet from the exact summand.

The endpoint jet is not a new fitted support summand; it is derived from the same primitive and the already frozen endpoint flags.

Physical wall pairing

On the source sheet inside the physical interval,

w=+i2s−an2.w=+i\sqrt{2s-an^2}.

The Kummer period is

∫−NNdnw=−iπa.\int_{-N}^{N}\frac{dn}{w} = -\frac{i\pi}{\sqrt a}.

The exact summand contributes only its source-prescribed endpoint regularization. Its finite parts vanish in the displayed odd principal parts. Therefore the generic regularized wall period is

Reg⁡∫−NNη0=−3iπ(x−y)(x+y)16(xy)4,\boxed{ \operatorname{Reg}\int_{-N}^{N}\eta_0 = -\frac{3i\pi(x-y)(x+y)}{16(xy)^4}, }

up to the common overall wavefunction normalization already omitted by the primary source. The sign uses the same positive sheet and lower-half-plane continuation as entries 226, 320.

Verdict

The continued exactness conjecture is falsified:

(−3,−2,−1,0)=(0,0,exact nonzero,nonzero Kummer relative class).\boxed{ (-3,-2,-1,0) = (0,0,\text{exact nonzero},\text{nonzero Kummer relative class}). }

The full occurrence lift first produces a genuine relative coefficient class at weight 00, one grade after the first nonzero Laurent coefficient.

This strengthens the sector-specific coefficient side of H2 without changing the carrier:

existing resolved carrier+higher-Rees relative Tate/Kummer coefficient data.\text{existing resolved carrier} + \text{higher-Rees relative Tate/Kummer coefficient data}.

Classification

Exact evidence

Next finite falsifier

Compute the monodromy and occurrence sewing of this new rank-one wall Kummer class before any absolute nine-master comparison.

Freeze the two cyclic occurrence orbits and transport

[dnw]\left[\frac{dn}{w}\right]

around the total-energy square-root loop. Test:

  1. its semisimple character under τ↦−τ\tau\mapsto-\tau;
  2. the induced action on the opposite endpoint polar jets;
  3. cyclic covariance among the 1212, 2323, and 3131 marked sectors;
  4. whether occurrence forgetting produces multiplicity two, cancellation, or a nontrivial sign local system.

A sewing failure inside the frozen relative coefficient object falsifies canonical global assembly but does not create a carrier. A need for a new incidence stratum would fire the shared-carrier falsifier.

Outcome contract

{
  "claim": "The complete weight-0 wall form is zero or meromorphically exact like the weight-minus-one form.",
  "status": "falsified",
  "normalized_residue": "3*n^2*(x-y)*(x+y)*(n^4*x^2*y^2-7*n^2*x*y*(x+y)+5*(x+y)^2)/(2*x*y*(n^2*x*y-2*x-2*y)^2)",
  "parity_in_n": "even",
  "punctured_wall_class": "3*(x-y)*(x+y)/(16*(x*y)^(7/2))*[dn/w]",
  "class_type": "rank-one Kummer",
  "endpoint_polar_jets": "opposite and source-derived",
  "generic_regularized_period": "-3*i*pi*(x-y)*(x+y)/(16*(x*y)^4)",
  "direct_elliptic_gysin_image": 0,
  "new_carrier_incidence": false,
  "next_experiment": "Compute monodromy and cyclic occurrence sewing of the weight-0 wall Kummer class."
}

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