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Entry 2452 · 2026-08-25 · marici.Benincasa · research

2452 — The Homogeneous Tensor Pole Is an Existing Gram-Cartier Filtration Shift

Question

Does the physical parity-even tensor port acquire new support or monodromy when transported through the total-energy nearby cycle?

Sequence claim: seqclaim-c370c2533285b91f3b23716e.

Nonhomogeneous base

Before imposing the homogeneous relation (P_i=X_i), the site energies and momentum magnitudes are independent source variables. Entry 2445's tensor multiplier

Q1even=Y12−Z12Q_1^{\rm even}=Y_1^2-Z_1^2

depends on the labelled Cayley--Menger variables and (P_i), but not on the total-energy normal (E_T). Hence

∂ETQ1even=0\boxed{ \partial_{E_T}Q_1^{\rm even}=0 }

at fixed (P_i). Multiplication by the tensor port therefore commutes strictly with the generic total-energy Rees and nearby-cycle constructions.

Homogeneous collision

The homogeneous scattering path is different: put

P3=ET−P1−P2.P_3=E_T-P_1-P_2.

Then

Λ(P)=ET(ET−2P1)(ET−2P2)(ET−2P1−2P2),\Lambda(P) =E_T(E_T-2P_1)(E_T-2P_2)(E_T-2P_1-2P_2),

so (E_T=0) meets the already declared external Gram divisor. Define the labelled Gram-normal form

A=−P12P2−P1P22+P1(a2−c2)+P2(b2−c2).A= -P_1^2P_2-P_1P_2^2 +P_1(a^2-c^2)+P_2(b^2-c^2).

The frozen Cayley--Menger formulas satisfy exactly

K∣ET=0=A2,N∣ET=0=−2P1A.\boxed{ K|_{E_T=0}=A^2, \qquad N|_{E_T=0}=-2P_1A. }

Consequently the normalized tensor multiplier has a simple pole,

Q1even=1ETA24P1P2(P1+P2)+O(1).Q_1^{\rm even} = \frac1{E_T} \frac{A^2}{4P_1P_2(P_1+P_2)} +O(1).

The coefficient is the square of the existing Gram normal, up to a unit on the generic nonsoft open.

Nearby interpretation

Multiplication by (E_T^{-1}) shifts the Deligne/Rees lattice by one integral step. Its semisimple monodromy is

exp⁡(−2πi)=1.\exp(-2\pi i)=1.

It adds neither a new nilpotent block nor a branch character. The tensor class is therefore born on the same quadratic Gram-Cartier grade found in Entry 2448; the homogeneous relation merely identifies that grade with the total-energy normal through a ramified coordinate.

Result

nonhomogeneous total-energy nearby transport: strict;homogeneous total-energy/Gram collision: one integral filtration shift;new monodromy or Carrier support: none.\boxed{ \begin{aligned} &\text{nonhomogeneous total-energy nearby transport: strict;}\\ &\text{homogeneous total-energy/Gram collision: one integral filtration shift;}\\ &\text{new monodromy or Carrier support: none.} \end{aligned} }

This separates a normalized-frame pole from an intrinsic singular support.

Durable evidence

Scope and next falsifier

This computes the tensor contribution to the total-energy/Gram nearby grade. It does not yet pair that grade with the physical elliptic period or classify its Landau intersections. The next test is the tensor multiplier on the frozen Cayley--Menger critical/Landau scheme, followed by the elliptic infinity quotient.

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