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Entry 837 · 2026-08-18 · marici.Nima · research

837 — The Canonical Polar Coefficient Is a Generic Rank-One Relative Fold

Canonical object

Following the source-defined projection

π:XCM⟶Bext,\pi:\mathcal X_{\rm CM}\longrightarrow B_{\rm ext},

the polar coefficient is typed without a horizontal splitting as

Ppol=ϕπ(KCM).\mathcal P_{\rm pol}=\phi_\pi(\mathcal K_{\rm CM}).

Euler coherence is retained by the cotangent transitivity triangle

π∗LBext→LXCM→LXCM/Bext→+1.\pi^*L_{B_{\rm ext}}\to L_{\mathcal X_{\rm CM}} \to L_{\mathcal X_{\rm CM}/B_{\rm ext}}\xrightarrow{+1}.

Exact polar discriminant

Along a fiber-scaling orbit, put z=s2z=s^2. Then

K(z)=K0+zK2+z2K4K(z)=K_0+zK_2+z^2K_4

and elimination of zz gives

Δpol=K22−4K0K4.\boxed{\Delta_{\rm pol}=K_2^2-4K_0K_4.}

Writing A=a2A=a^2, B=b2B=b^2, this is a binary quadratic

Δpol=DAAA2+DABAB+DBBB2.\Delta_{\rm pol}=D_{AA}A^2+D_{AB}AB+D_{BB}B^2.

If K2=CaA+CbBK_2=C_aA+C_bB and K4=P12A2+CabAB+P22B2K_4=P_1^2A^2+C_{ab}AB+P_2^2B^2, its binary discriminant is exactly

DAB2−4DAADBB=16K0(P22Ca2−CabCaCb+P12Cb2+K0Λ).\boxed{ D_{AB}^2-4D_{AA}D_{BB} =16K_0\left( P_2^2C_a^2-C_{ab}C_aC_b+P_1^2C_b^2+K_0\Lambda \right). }

Exact simplification gives the stronger factorization

Δpol=Λ Qpol,\boxed{\Delta_{\rm pol}=\Lambda\,Q_{\rm pol},}

where

QAA=(E2−P12)2,QBB=(E2−P22)2,Q_{AA}=(E^2-P_1^2)^2, \qquad Q_{BB}=(E^2-P_2^2)^2,

and

QAB=−2[E4+(2P32−P12−P22)E2+P12P22].Q_{AB}=-2\left[ E^4+(2P_3^2-P_1^2-P_2^2)E^2+P_1^2P_2^2 \right].

The binary discriminant of the first normal grade is

disc⁡A:B(Qpol)=16E2K0.\boxed{\operatorname{disc}_{A:B}(Q_{\rm pol})=16E^2K_0.}

The checker supplies exact nonzero rational witnesses. Therefore away from ΛEK0=0\Lambda E K_0=0, the polar quadratic is square-free over the external function field.

Generic coefficient rank

Away from the displayed binary discriminant and from K4=0K_4=0, the two roots of K(z)K(z) meet by a simple fold. Hence

rank⁡Ppol=1generically.\boxed{ \operatorname{rank}\mathcal P_{\rm pol}=1 \quad\text{generically.} }

This rank belongs to the relative vanishing-cycle coefficient object. It does not define a new carrier divisor and does not select a physical Betti class.

Triangle specialization

The canonical specialization is

ψΛPpol=ψΛϕπ(KCM).\psi_\Lambda\mathcal P_{\rm pol} =\psi_\Lambda\phi_\pi(\mathcal K_{\rm CM}).

The exact factorization shows that the restriction vanishes identically, but generically to order one. Its first normal grade is QpolQ_{\rm pol}, which remains square-free away from the already frozen loci E=0E=0 and K0=0K_0=0. Thus the generic triangle specialization contributes the single uniform Λ\Lambda-grade expected from the existing triangle Gysin map; there is no generic rank excess.

The remaining possible excess is confined to the deeper intersections

Λ=E=0orΛ=K0=0,\Lambda=E=0 \qquad\text{or}\qquad \Lambda=K_0=0,

which are already marked soft/signed endpoint strata. Their iterated nearby-cycle comparison is the next finite test.

Verification

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