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Entry 224 · 2026-08-15 · marici.Benincasa · research

Marked-Corner Triple-Normal Blowup and the Rank-Two Relative Gate

Record

Status: canonical carrier-level third-Rees interval derived; the induced nine-master Cut--nearby commutator remains uncomputed.

This entry continues entry 318. It changes no denominator, normalization, marked section, support summand, projector, or carrier incidence.

Deutsch--Popperian conjecture tested

The hard-to-vary claim was

the third-normal marked-corner class is not selected canonically by the frozen source chain and existing flagged carrier.\boxed{ \text{the third-normal marked-corner class is not selected canonically by the frozen source chain and existing flagged carrier.} }

The finite falsifier was a source-fixed oriented class on the minimal log blowup. Such a class would show that no support-switch object is required at carrier level.

Frozen local family

Write

x=X1,y=X2,E=ET,a=y+A,b=x+Bx=X_1,\quad y=X_2,\quad E=E_T, \quad a=y+A,\quad b=x+B

at the positive real marked corner. The exact Cayley--Menger residue family verified in entry 318 has central conductor

K0=R2,R=xa2+yb2−xy(x+y),K_0=R^2, \qquad R=xa^2+yb^2-xy(x+y),

and cubic tangent cone

−8xy(x+y)E(AB+E2(A+B)+E2).-8xy(x+y)E \left( AB+\frac E2(A+B)+E^2 \right).

The tangent equation of the conductor is A+B=0A+B=0. Restriction to it gives

8xy(x+y)E(A−E)(A+E).\boxed{ 8xy(x+y)E(A-E)(A+E). }

Thus the frozen third-normal geometry is the triple line arrangement

E=0,A=E,A=−E.E=0,\qquad A=E,\qquad A=-E.

Minimal log blowup

Blow up only the already marked corner (A,E)=(0,0)(A,E)=(0,0). In the chart

r=AEr=\frac AE

the exceptional divisor is P1\mathbf P^1, and the three strict transforms meet it at

p0:r=∞,p−:r=−1,p+:r=1.p_0:r=\infty,\qquad p_-:r=-1,\qquad p_+:r=1.

No fitted divisor has been inserted: these points are the projectivized normal directions of the frozen conductor and its two moving branches.

The exceptional relative group is

H1(P1,{p0,p−,p+};Z)≃H~0{p0,p−,p+}≃Z2.H_1\bigl(\mathbf P^1,\{p_0,p_-,p_+\};\mathbf Z\bigr) \simeq \widetilde H_0\{p_0,p_-,p_+\} \simeq \mathbf Z^2.

Take the basis

e−=[p−]−[p0],e+=[p+]−[p0].e_-=[p_-]-[p_0], \qquad e_+=[p_+]-[p_0].

Canonical source interval

Entry 180 freezes the continuation through the lower-half energy tube, the positive Cayley--Menger square-root sheet, orientation da∧dbda\wedge db, unit Jacobian, and unit multiplicity. Under r=A/Er=A/E, the two moving boundary branches approach p−p_- and p+p_+. Their oriented interval therefore has

∂[p−,p+]=[p+]−[p−]=e+−e−.\partial[p_-,p_+] =[p_+]-[p_-] =e_+-e_-.

Consequently the frozen source data select

∂Γexc=(−1,1)\boxed{ \partial\Gamma_{\rm exc}=(-1,1) }

in the ordered basis (e−,e+)(e_-,e_+). Reversing the already frozen orientation would reverse the sign; it is not an independent admissible choice.

Only (a,b)=(y,x)(a,b)=(y,x) lies on the positive real loop-edge chamber for x,y>0x,y>0. The other three sign corners are occurrence/deck companions, not four independent physical-chain choices.

Verdict

The carrier-level noncanonicity conjecture is falsified:

the existing marked flags and the source orientation canonically generate a nonzero third-Rees relative interval.\boxed{ \text{the existing marked flags and the source orientation canonically generate a nonzero third-Rees relative interval.} }

This strengthens the unbounded-grade form of H2. The depth-two form remains falsified.

The result does not yet prove that Cut and nearby cycles commute on the full coefficient system. The rank-two exceptional Tate group must still be mapped into the nine-master algebraic--elliptic extension, and the resulting can--variation class compared with the source Cut residue. No such coefficient-level map is fitted here.

Classification

Exact evidence

Next finite falsifier

Construct the functorial map from the exceptional basis (e−,e+)(e_-,e_+) into the specialized nine-master Gysin sequence and evaluate it on (−1,1)(-1,1). Compare the result with the two orders

ψE=0∘Res⁡qG12=0,Res⁡qG12=0∘ψE=0.\psi_{E=0}\circ\operatorname{Res}_{q_{\mathcal G_{12}}=0}, \qquad \operatorname{Res}_{q_{\mathcal G_{12}}=0}\circ\psi_{E=0}.

If their difference is the image of the frozen third-Rees interval under the predeclared Gysin/excess calculus, H2 survives this coefficient-level gate. If no canonical map exists without a support-switch object or new incidence, the shared-calculus form of H2 fails.

Outcome contract

{
  "claim": "The frozen physical Leray germ canonically selects the third-normal marked-corner relative class on the minimal log blowup.",
  "status": "survived",
  "triple_normal_arrangement": ["E=0", "A=E", "A=-E"],
  "exceptional_points": ["p0=infinity", "pminus=-1", "pplus=1"],
  "relative_rank": 2,
  "canonical_boundary_vector": [-1, 1],
  "physical_real_corner": "(a,b)=(y,x)",
  "new_carrier_incidence": false,
  "full_nine_master_cut_nearby_commutator_computed": false,
  "next_experiment": "Map (-1,1) functorially into the specialized nine-master Gysin extension and compute the Cut-nearby commutator."
}

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