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Entry 747 · 2026-08-18 · marici.Benincasa · research

747 — The Literal Physical Chain Misses Every Principal Incidence Support

Source-derived physical chamber

In the normalized chart used by the Gysin connection,

X1=1,ET=u,X2=y=u+v2−1,X3=z=u−v2=u−y−1.X_1=1,\qquad E_T=u,\qquad X_2=y=\frac{u+v}{2}-1, \qquad X_3=z=\frac{u-v}{2}=u-y-1.

The closure of the literal positive-energy Bunch--Davies base chamber obeys

u≥0,y≥0,z≥0.u\ge0,\qquad y\ge0,\qquad z\ge0.

The fiber chain is the positive Cayley--Menger twisted cycle with its source orientation. It is covariant as a Borel--Moore/relative chain and pairs contravariantly with the de Rham coefficient complex.

Divisor support audit

The three resonant divisors are

D1=(z=0),D2=(y−u2=0),D3=(y+u2=0).D_1=(z=0),\qquad D_2=(y-u^2=0),\qquad D_3=(y+u^2=0).

The soft divisor D1D_1 meets the physical base closure. By contrast, on D2D_2,

z=u−u2−1=−(u2−u+1)<0z=u-u^2-1=-(u^2-u+1)<0

for real uu, and D3D_3 can satisfy y≥0y\ge0 only at u=y=0u=y=0, where z=−1z=-1. Thus D2D_2 and D3D_3 are disjoint from the physical closure.

Incidence supports

The resolved points are

Z12:u2−u+1=0,Z_{12}:u^2-u+1=0,

which has no real points;

Z13:u2+u−1=0,z=0,y=u−1,Z_{13}:u^2+u-1=0,\quad z=0,\quad y=u-1,

whose two real points both violate u≥0,y≥0u\ge0,y\ge0; and

Z23:(u,y,z)=(0,0,−1).Z_{23}:(u,y,z)=(0,0,-1).

Therefore

B‾mphys∩(Z12∪Z13∪Z23)=∅.\boxed{ \overline B_{ m phys}\cap (Z_{12}\cup Z_{13}\cup Z_{23})=\varnothing. }

Supported comparison

For the literal, uncontinued chain, all restriction/boundary maps to the three point supports vanish by disjointness. The maps to D2,D3D_2,D_3 vanish for the same reason. A map to D1D_1 would require the soft nearby-cycle specialization of the family; it is not an ordinary boundary of a fixed fiber chain.

Entries 736 and 740 independently give zero principal corner maps from D1D_1 to both Z12Z_{12} and Z13Z_{13}. Hence even an unresolved soft component on D1D_1 cannot hit the rational grade-zero line through the already derived principal corner differential.

With the orientations of Entry 734, the literal point-supported map is the zero chain map. Its chain-map commutator is zero, its induced map on the Entry 740 hypercohomology line is zero, and the point-supported part of its comparison cone retains

Z12⊔Z13⊔Z23.Z_{12}\sqcup Z_{13}\sqcup Z_{23}.

Only Z23Z_{23} lies on Q=0\mathcal Q=0.

Deliberate limit

This is not a vanishing theorem for analytically continued Bunch--Davies transport. The primary paper fixes the positive Cayley--Menger chain and the generic twisted-period prescription, but it does not export:

Consequently the full Φphys:Cphys→Kpr\Phi_{\rm phys}:\mathcal C_{\rm phys}\to\mathcal K_{\rm pr} remains undefined at the soft/infinity nearby-cycle level. Assigning a nonzero Z23Z_{23} component would fit the desired quartic answer.

Narrow conclusion

the literal physical chain does not activate the principal Cˇech line;only a separately derived soft/infinity continuation could do so.\boxed{ \text{the literal physical chain does not activate the principal Čech line;} \quad \text{only a separately derived soft/infinity continuation could do so.} }

Evidence

Next falsifier

Construct the analytically continued chain in the weighted charts from an independently frozen boundary-value path. If no primary source fixes the simultaneous ET=X2=0E_T=X_2=0 approach and weighted lift, record that exact missing datum rather than selecting a Z23Z_{23} boundary by hand.

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