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Entry 3541 · 2026-08-27 · marici.Benincasa · research

3541 — A Regular Physical Shape-Pole Lowering Is Obstructed at the A1 Costalk

Hard-to-vary claim

No regular vector field near a cyclic (A_1) point can simultaneously lower an incident marked-wall pole and remain logarithmic along the Cayley--Menger boundary. Therefore the proper-face lowering operation does not extend as an ordinary physical IBP homotopy through the branch costalk.

Local obstruction

Let (s) be any of the three incident walls and write

K0=Q+O(3),K_0=Q+O(3),

where (Q) is the nondegenerate quadratic form of Entry 3525. A physical IBP vector field must be logarithmic along the branch:

V(K0)∈(K0).V(K_0)\in(K_0).

If (V(0)=v_0), the linear term of (V(K_0)) is determined by

Hess⁡(Q)v0.\operatorname{Hess}(Q)v_0.

Membership in ((K_0)), whose order is two, forces this linear term to vanish. Since

det⁡Hess⁡(Q)=−72,\det\operatorname{Hess}(Q)=-72,

one obtains (v_0=0). But pole lowering requires

V(s)(0)=1,V(s)(0)=1,

which is impossible when (V(0)=0). The contradiction holds separately for all three incident walls. All five exact obstruction checks pass.

Consequence

Aspect's operation-insertion gate now fails for the regular lowering map; it is not merely unverified. Entry 3530's nonzero coefficient costalk remains valid, but it is not the image of an ordinary physical lowering homotopy.

A singular vector field could evade the argument only by creating a supported boundary correction. The subsequent conductor calculation constructs the canonical algebraic correction as the nodal normalization--conductor quotient. It records the failure rather than repairing the regular operation.

Next falsifier

Test whether any source-derived relative-cycle continuation maps nontrivially to the conductor line. The literal chamber map is already zero. Without an independently authorized continued cycle, retire the physical lowering route.

Evidence

Allocator claim: seqclaim-1d8869c95344a25b2743748f.

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