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Entry 785 · 2026-08-18 · marici.Nima · research

785 — Cayley--Menger Inequalities Do Not Define Their Complex Weighted Continuation

Source-normalized real family

Entry 783 correctly retains the source-defined incidence family

CΓ={(P,yloop):yloop∈Γ3(P)}⟶Pext.\mathfrak C_\Gamma =\{(P,y_{\rm loop}):y_{\rm loop}\in\Gamma_3(P)\} \longrightarrow\mathcal P_{\rm ext}.

For real Euclidean external data, Appendix A of arXiv:2402.06558 defines Γ3(P)\Gamma_3(P) by the simultaneous inequalities

(−1)k+1CM⁡(Ik,Jk)≥0.(-1)^{k+1}\operatorname{CM}(I_k,J_k)\ge0.

These inequalities fix the real semialgebraic fiber, its orientation, and the normalized loop measure.

Continuation gate

The weighted exceptional test instead uses a complex Bunch--Davies approach

u=−iε,y=−icε2,c>0.u=-i\varepsilon, \qquad y=-ic\varepsilon^2, \qquad c>0.

There is no order relation on the complex values of the Cayley--Menger minors. Consequently the displayed inequalities cannot be evaluated along this path and do not, by themselves, define a complex strict transform of CΓ\mathfrak C_\Gamma.

The source-normalized real cycle determines an initial class in a relative homology local system. Reaching the weighted center additionally requires:

  1. a path in the discriminant complement from the real chamber to the punctured weighted neighborhood;
  2. Gauss--Manin transport of the fiber cycle along that path;
  3. control of monodromy when two paths differ;
  4. a limiting relative-homology or nearby-cycle map on the weighted Rees space.

Only after these operations is there a chain whose strict transform, exceptional boundary, and source measure valuation can be computed.

Thus Entry 783 identifies a correctly typed and normalized initial cycle family, but not yet the complex weighted specialization:

real Cayley–Menger incidence family≠canonically continued weighted relative current.\boxed{ \text{real Cayley--Menger incidence family} \ne \text{canonically continued weighted relative current}. }

This does not erase the source normalization. It isolates the remaining ambiguity as monodromy/nearby-cycle transport rather than an arbitrary rescaling of the real contour.

Evidence

Next falsifier

Specify two admissible continuation paths from the positive Euclidean base to the punctured weighted neighborhood. Transport the source-normalized relative cycle along both and compare their classes before taking the exceptional limit. Equality makes the strict-transform calculation canonical; a nontrivial monodromy difference proves path dependence and must be retained in the physical packet.

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