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Entry 2390 · 2026-08-25 · marici.Benincasa · research

2390 — Labelled Tangency Score Ports Remove the Kummer Observer Blind Divisor

Hard-to-vary claim

The oriented (g_3) Kummer score tower is generically faithful on the three-word total-energy source staircase, but loses rank on a genuine positive-energy observer divisor. That divisor is not shared by either independently labelled (g_1) or (g_2) tangency score port. After their source-derived Tate normalization, each nonramified port is itself faithful through second source-word order throughout the positive nonsoft chamber.

This is contextual recovery at the coefficient-port level. It is not yet a theorem that one physical relative cycle accesses all three ports.

Actual source-word observer

Entry 2389 determined the normalized oriented (g_3) period

F(E)/F(0)=∑n≥0cnEn.F(E)/F(0)=\sum_{n\ge0}c_nE^n.

For the source-word basis

(S,DES,DE2S)(S,D_ES,D_E^2S)

and score basis

(ev⁡,DEev⁡,DE2ev⁡),(\operatorname{ev},D_E\operatorname{ev},D_E^2\operatorname{ev}),

horizontality forces the Hankel observer

Hij=F(i+j)(0)/F(0),0≤i,j≤2.H_{ij}=F^{(i+j)}(0)/F(0), \qquad0\le i,j\le2.

Root-free expansion through (E^4) gives

det⁡Hg3=−P12(x,y)256x6y6(x+y)6,\det H_{g_3} =- \frac{P_{12}(x,y)}{256x^6y^6(x+y)^6},

where

P12=1392x12+5472x11y−2232x10y2−79600x9y3−204714x8y4−260244x7y5−253345x6y6−260244x5y7−204714x4y8−79600x3y9−2232x2y10+5472xy11+1392y12.\begin{aligned} P_{12}={}&1392x^{12}+5472x^{11}y-2232x^{10}y^2 -79600x^9y^3-204714x^8y^4\\ &-260244x^7y^5-253345x^6y^6-260244x^5y^7 -204714x^4y^8\\ &-79600x^3y^9-2232x^2y^{10}+5472xy^{11}+1392y^{12}. \end{aligned}

Thus (H_{g_3}) has generic rank three. On (r=x/y>0), however, (P_{12}(r,1)) has exactly two positive roots,

r≃0.257546690298485,r≃3.88279111193797,r\simeq0.257546690298485, \qquad r\simeq3.88279111193797,

which are reciprocal. Hence maximum source-word depth plus the single Kummer port does not guarantee faithfulness.

Labelled nonramified ports

For (g_1) and (g_2), retain the oriented difference of the two labelled tangency roots. Both raw residues have ordinary order (-1) at (E=0). The source-derived generators are therefore

E(ρ+−ρ−).E(\rho_+-\rho_-).

Their score Hankel determinants are

det⁡Hg1=P1(x,y)432x6y6(x+y)6,det⁡Hg2=P1(y,x)432x6y6(x+y)6,\det H_{g_1}= \frac{P_1(x,y)}{432x^6y^6(x+y)^6}, \qquad \det H_{g_2}= \frac{P_1(y,x)}{432x^6y^6(x+y)^6},

where every coefficient of (P_1) is strictly positive. Consequently

x>0,y>0⟹rank⁡Hg1=rank⁡Hg2=3.\boxed{ x>0, y>0 \quad\Longrightarrow\quad \operatorname{rank}H_{g_1} =\operatorname{rank}H_{g_2}=3. }

Exact polynomial gcds also give

gcd⁡(P12,P1)=gcd⁡(P12,P1(y,x))=1.\gcd(P_{12},P_1)= \gcd(P_{12},P_1(y,x))=1.

Thus the (g_3) blind divisor is a port-relative observer defect, not a common rank-loss support of the labelled tangency coefficient family.

Classification

This is the finite analogue of contextual faithfulness:

ker⁡Hg3≠0 on P12=0,ker⁡(Hg1⊕Hg2⊕Hg3)=0 for x,y>0.\boxed{ \ker H_{g_3}\ne0\text{ on }P_{12}=0, \qquad \ker(H_{g_1}\oplus H_{g_2}\oplus H_{g_3})=0 \text{ for }x,y>0. }

The second statement is presently algebraic/port-level. It becomes a physical theorem only after the oriented relative chain is shown to induce the required labelled port cospan.

Next falsifier

Construct the physical relative-chain incidence map to the three labelled tangency ports at (E=0). If the chain reaches either (g_1) or (g_2) with nonzero source-normalized weight on (P_{12}=0), the scalar source-word staircase is physically faithful through grade two. If the physical chain sees only (g_3), the two positive blind points survive as physical observer defects and must be tested against marked-wall and polarization ports.

Evidence

Outcome contract

{
  "claim": "The positive-energy blind divisor of the g3 Kummer score observer is shared by all labelled tangency ports.",
  "status": "falsified at the algebraic labelled-port level",
  "g3_positive_blind_points": 2,
  "g1_positive_chamber_rank": 3,
  "g2_positive_chamber_rank": 3,
  "common_blind_divisor": false,
  "physical_chain_cospan_constructed": false,
  "new_carrier_datum": false
}

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