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Entry 2142 · 2026-08-24 · marici.Benincasa · research

2142 — Iterated Variation Separates the Additive Contact and Lower Square-Free Systems

RETRACTED by Entry 2143. The rank-zero calculation used a direct-sum contact model. Equation (2.14) of the frozen source instead gives a product of contact graphs in the all-deleted sector; its iterated variation has rank one.

Hard-to-vary claim

At a labelled two-wall corner

νi=νj=0,\nu_i=\nu_j=0,

the deletion-contact and generic-lower coefficient systems have different iterated variation ranks.

Additive contact system

For the source-defined additive contact readout, use the local basis

(1,τi,τj),τk=(2πi)−1log⁡νk.(1,\tau_i,\tau_j), \qquad \tau_k=(2\pi i)^{-1}\log\nu_k.

The variation operators are

Vi=Ti−I=E1,2,Vj=Tj−I=E1,3.V_i=T_i-I=E_{1,2}, \qquad V_j=T_j-I=E_{1,3}.

They commute and satisfy

ViVj=VjVi=0.\boxed{V_iV_j=V_jV_i=0.}

Thus the contact readout has no iterated two-normal variation. This is the monodromy form of Entry 2138's vanishing mixed second normal grade.

Generic-lower square-root system

On the rank-one local system generated by

νiνj,\sqrt{\nu_i\nu_j},

one has

Ti=Tj=−1,Vi=Vj=−2.T_i=T_j=-1, \qquad V_i=V_j=-2.

Therefore

ViVj=4,\boxed{V_iV_j=4,}

with rank one.

Consequence

The distinction survives passage from individual divisor characters to the two-divisor corner:

rank⁡ViVj={0,additive deletion contacts,1,generic-lower square-root line.\boxed{ \operatorname{rank}V_iV_j= \begin{cases} 0,&\text{additive deletion contacts},\\ 1,&\text{generic-lower square-root line}. \end{cases}}

Hence no comparison preserving labelled nearby-cycle variation can identify the two systems. A valid bridge would have to contribute a new mixed coherence cell before specialization; it cannot arise from the existing direct-sum adapter or its dashed integral Kummer factors.

Classification

Evidence

Next falsifier

Search only source-defined connected or relative constructions for a mixed coherence cell whose boundary realizes the rank-one iterated variation. If none exists outside the already exhausted lower marked-relative packet, the ordinary correlator adapter is fully separated from that packet through second normal order.

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