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Entry 39 · 2026-08-13 · marici.Nima · research

Scalar-Derived Worldsheet Class and Pre-Pairing Factorization

Record

Date: 2026-08-13

Status: corrected in part by entries 70--75. The complete Parke--Taylor period vector and derived Verdier perfectness still identify the representation-independent cohomology class

Jn=[(Pf⁡′An)2].\boxed{ \mathsf J_n = [(\operatorname{Pf}'A_n)^2]. }

The equality is representation independent and is separated by a complete Parke--Taylor basis. However, the stronger claim that a complete occurrence-decorated scalar covector already factorizes in the facewise Pochhammer/Cousin complex before index raising is conditional. Entry 38 supplies that comparison on transverse cells. For the eight nontransverse pentagons, entries 74--75 now supply a formal scalar-edge Cousin counit, the correct weighted target cube, and one normalized torsion-free local derived class. Entry 76 proves that the caps and cube are actual scalar faces and that their polynomial extension closes. The remaining chain-level datum is the dependent route-to-belt Beck--Chevalley attachment.

Thus this entry contains two logically distinct results:

  1. the cohomological half-class and its Pfaffian-square identification remain established;
  2. its claimed intrinsic scalar chain provenance and pre-pairing coherent factorization are proved only on the transverse subcomplex.

Forward refinement (entries 82--83): target-first support descent now closes the local dependent rank-two symbols, and the fixed-mark contact transport maps facewise to a loaded chain with vanishing octagonal contact class. The remaining chain-level qualification in item 2 concerns global horizontal assembly of the unmarked/full-symbol coefficient summands. It is not a remaining obstruction in the marked contact sector.

Forward correction (entry 84): pole-grade exhaustion shows that there is no unmarked/full-symbol remainder in the eight-point polarity difference. The double-pole sector cancels pointwise, the single-pole sector is exhausted by lower-point factorization triangles, and the regular sector is the marked transport of entry 83. The complete PC polarity homotopy is still conditional, but for a different reason: the saturated six-point tripod has one core-changing occurrence/Gysin entry counit not covered by the transverse comparison theorem. Entry 85 reduces the resulting closed residue class to one undetermined scalar multiplying the primitive factorized line. Global gluing of the primitive local half-lines remains a separate higher-coherence problem rather than an omitted coefficient sector.

The finite-α′\alpha' object is a regulator lift. Its full α′\alpha'-dependent class is not claimed to equal the undeformed Pfaffian square; the equality is for the normalized field-theory/nearby-cycle class that defines the CHY half-object.

Correct derived typing

Let

Hn−=Hn−3(Mn,∇−ωn),Hn+=Hn−3(Mn,∇ωn),H_n^- = H^{n-3}(M_n,\nabla_{-\omega_n}), \qquad H_n^+ = H^{n-3}(M_n,\nabla_{\omega_n}),

and let

In:Hn−⊗Hn+⟶KnI_n: H_n^-\otimes H_n^+ \longrightarrow K_n

be the generic twisted-intersection pairing. Its flat map is

In♭:Hn+→∼(Hn−)∗.I_n^\flat: H_n^+ \xrightarrow{\sim} (H_n^-)^*.

At chain level the canonical object is the Verdier pairing

In:RΓc(Mn,DR⁡L−ωn)⊗LRΓ(Mn,DR⁡Lωn)⟶Kn[−2(n−3)].\mathbb I_n: R\Gamma_c \bigl(M_n,\operatorname{DR}\mathscr L_{-\omega_n}\bigr) \overset L\otimes R\Gamma \bigl(M_n,\operatorname{DR}\mathscr L_{\omega_n}\bigr) \longrightarrow K_n[-2(n-3)].

Entry 38 gives a finite, facewise model for the compact/normal-cone side. It does not choose an inverse between arbitrary point-set dg models. The index raising used here is therefore

(In♭)−1(\mathbb I_n^\flat)^{-1}

in the derived category, whose middle-cohomology map is the familiar inverse BAS/KLT pairing.

This distinction removes the apparent conflict between a canonical class and a noncanonical smooth representative.

The scalar Pochhammer covector

For each cyclic order α\alpha, let

Ξn,αsc∈C∗cell(AssEnv⁡α;LJ)\Xi^{\rm sc}_{n,\alpha} \in C_*^{\rm cell} \bigl(\operatorname{AssEnv}_\alpha;\mathcal L_J\bigr)

be the complete occurrence-resolved scalar associated-grade element. On the transverse occurrence-decorated subcomplex, apply the comparison of entry 38:

Ξn,α′PC(α)=χα′Ξn,αsc.\Xi^{\rm PC}_{n,\alpha'}(\alpha) = \chi_{\alpha'}\Xi^{\rm sc}_{n,\alpha}.

As a formula on the complete decorated complex, this line is now a target rather than a theorem. The missing components are the eight-point route pentagons and their higher-arity analogues. The undecorated Pochhammer face map exists there, but its scalar occurrence coefficient has not been lifted.

Let

FT⁡\operatorname{FT}

denote the normalized field-theory symbol: take the leading normal-torus/Pochhammer grade and replace

2πiα′e2πiα′XE−1\frac{2\pi i\alpha'} {e^{2\pi i\alpha'X_E}-1}

by its VEV_E-leading term 1/XE1/X_E. The generalized Pochhammer field-theory localization is vertexwise. A maximal-codimension face labelled by a triangulation TT contributes the scalar cubic denominator

ϵT∏E∈TXE.\frac{\epsilon_T}{\prod_{E\in T}X_E}.

The scalar associated grade acts on these vertex coefficients before the Pochhammer regularization. Consequently

⟨PT⁡α−,FT⁡Ξn,α′PC⟩=aR,n(α).\boxed{ \left\langle \operatorname{PT}^-_\alpha, \operatorname{FT}\Xi^{\rm PC}_{n,\alpha'} \right\rangle = a_{R,n}(\alpha). }

The period equality is exact. Its interpretation as the period of one globally assembled cell-resolved Pochhammer chain is conditional on completing the nontransverse coefficient lift. Independently, entries 14 and 27 provide the order-indexed scalar grade and its marked regional summands, so the period vector itself does not depend on that unfinished assembly.

The direct scalar descent theorem of entry 14 says that the family aR,n(α)a_{R,n}(\alpha) annihilates the Parke--Taylor kernel. Hence these periods define a representation-independent derived covector

AR,n∈(Hn−)∗.A_{R,n} \in (H_n^-)^*.

Derived index raising

Define

Jn=(In♭)−1AR,n∈Hn+.\boxed{ \mathsf J_n = (I_n^\flat)^{-1}A_{R,n} \in H_n^+. }

Equivalently, this is the middle-cohomology index raising of the scalar period covector. Once the nontransverse lift is completed, it should also be the image of one globally assembled facewise Pochhammer/Cousin covector.

Choose any genuine BCJ-sized Parke--Taylor bases B−⊂Hn−B_-\subset H_n^- and B+⊂Hn+B_+\subset H_n^+. The coordinate expression is

Jn=∑β∈B+PT⁡β+(m−1)βαaR,n(α).\mathsf J_n = \sum_{\beta\in B_+} \operatorname{PT}^+_\beta (m^{-1})^{\beta\alpha} a_{R,n}(\alpha).

Because this is the coordinate expression of a derived duality morphism, changes of either basis give the same class. No pseudoinverse of the full ordering matrix is used.

Identification with the Pfaffian square

The CHY NLSM formula states

In ⁣(PT⁡α−,[(Pf⁡′An)2])=AnNLSM(α).I_n\!\left( \operatorname{PT}^-_\alpha, [(\operatorname{Pf}'A_n)^2] \right) = A_n^{\rm NLSM}(\alpha).

The scalar normal-grade theorem gives

aR,n(α)=AnNLSM(α)a_{R,n}(\alpha) = A_n^{\rm NLSM}(\alpha)

for every even cyclic order, while both sides vanish at odd multiplicity. Therefore, for every α∈B−\alpha\in B_-,

In ⁣(PT⁡α−,Jn)=In ⁣(PT⁡α−,[(Pf⁡′An)2]).I_n\!\left( \operatorname{PT}^-_\alpha, \mathsf J_n \right) = I_n\!\left( \operatorname{PT}^-_\alpha, [(\operatorname{Pf}'A_n)^2] \right).

Perfectness separates the two classes:

Jn=[(Pf⁡′An)2]∈Hn+.\boxed{ \mathsf J_n = [(\operatorname{Pf}'A_n)^2] \in H_n^+. }

This cohomological conclusion is the sound part of the claimed provenance. Until the nontransverse coefficient lift is completed, the covector on the left is canonically specified by its scalar-derived Parke--Taylor periods, not yet by one complete occurrence-decorated worldsheet chain.

Factorization before pairing

Let ee be an allowed physical channel. The scalar occurrence coaction is

Ge(h)=−Xde0Xehe0−Xde1Xehe1.G_e(h) = -\frac{X_{d_e^0}}{X_e}h_e^0 -\frac{X_{d_e^1}}{X_e}h_e^1.

Entry 38 lifts it before any pairing on its proved transverse domain:

dPCGeα′=Geα′dPC,d_{\rm PC}G_e^{\alpha'} = G_e^{\alpha'}d_{\rm PC},

and proves the normalized specialization law

gr⁡Ve−1Res⁡ePCχα′=(χα′,L⊠χα′,R)Ge.\boxed{ \operatorname{gr}_{V_e}^{-1} \operatorname{Res}^{\rm PC}_e \chi_{\alpha'} = (\chi_{\alpha',L}\boxtimes\chi_{\alpha',R}) G_e. }

The right-hand side already contains:

  1. the physical channel;
  2. the oriented normal line;
  3. the two source slots;
  4. one scalar contact mark in every resulting component;
  5. the lower-point product cell;
  6. the 1/Xe1/X_e propagator.

No Parke--Taylor factor and no inverse KLT kernel has entered.

On the transverse occurrence-decorated subcomplex this gives the local factorization law. The desired extension to the complete scalar element is

gr⁡Ve−1Res⁡ePCAR,nPC=AR,LPC⊠AR,RPC.\boxed{ \operatorname{gr}_{V_e}^{-1} \operatorname{Res}^{\rm PC}_e A^{\rm PC}_{R,n} = A^{\rm PC}_{R,L} \boxtimes A^{\rm PC}_{R,R}. }

Forbidden parity channels have no supported leading normal symbol, so both sides vanish.

For a nested cut set EE, normal-crossing monoidality and strict cut commutativity give

gr⁡VERes⁡EPCAR,nPC=⊠R∈R(E)ARPC.\operatorname{gr}_{V_E} \operatorname{Res}^{\rm PC}_E A^{\rm PC}_{R,n} = \boxtimes_{R\in\mathcal R(E)} A^{\rm PC}_{R}.

These are the required factorization formulas, but their assertion on one globally assembled occurrence-decorated chain is conditional on the nontransverse Cousin lift. At cohomology level the same factorization follows independently from the identified Pfaffian-square class and its standard boundary degeneration.

Index raising on the channel quotient

At Xe=0X_e=0, the full generic pairing is resonant and its full residue matrix is rank deficient. Do not invert it.

The boundary Verdier pairing instead restricts to the induced channel quotient:

gr⁡VeIn=ϵe (IL⊠IR),\operatorname{gr}_{V_e}\mathbb I_n = \epsilon_e\, (\mathbb I_L\boxtimes\mathbb I_R),

with ϵe\epsilon_e the plumbing-normal orientation sign. Applying derived duality only on this quotient gives

Δe+Jn=JL⊠JR.\boxed{ \Delta_e^+\mathsf J_n = \mathsf J_L\boxtimes\mathsf J_R. }

This conclusion follows from the pre-pairing covector factorization and perfectness of the two lower-point pairings. It is not obtained by inverting Res⁡emn\operatorname{Res}_e m_n on the full nn-point space.

The reduced-Pfaffian degeneration supplies an independent representative-level check:

(Pf⁡′An)2⟶(Pf⁡′AL)2(Pf⁡′AR)2(\operatorname{Pf}'A_n)^2 \longrightarrow (\operatorname{Pf}'A_L)^2 (\operatorname{Pf}'A_R)^2

with the appropriate plumbing power in allowed channels and zero leading term in forbidden channels.

Natural factorization verdict

The original falsification question was whether

Iscalar−1gr⁡RAscalarI_{\rm scalar}^{-1} \operatorname{gr}_R A_{\rm scalar}

was merely an amplitude reconstruction device.

At cohomology level it is not: the complete scalar-derived period covector determines a unique half-class. At chain level the stronger answer remains conditional. The intended sequence is

gr⁡RAscalar⟶Ξsc⇢χα′ΞPC→FT⁡ARPC→(I♭)−1J,\operatorname{gr}_R A_{\rm scalar} \longrightarrow \Xi^{\rm sc} \overset{\chi_{\alpha'}}{\dashrightarrow} \Xi^{\rm PC} \xrightarrow{\operatorname{FT}} A_R^{\rm PC} \xrightarrow{(I^\flat)^{-1}} \mathsf J,

where the dashed arrow is proved on transverse cells and still requires the nontransverse scalar-facet lift. The factorization square commutes at the ΞPC\Xi^{\rm PC} stage on that proved domain and after passing to the identified cohomology class. It has not yet been assembled as a globally coherent pre-pairing chain map.

Thus the half-object exists canonically in cohomology. The stronger statement that its complete factorization law is already intrinsic before pairing is the live pentagon/Cousin frontier.

Consequences for the three-generator web

With twist reversal understood,

J+=[(Pf⁡′A)2],J−∈H−.\mathsf J^+ = [(\operatorname{Pf}'A)^2], \qquad \mathsf J^-\in H^-.

Therefore the standard scalar-derived pairings remain

⟨C,J⟩=NLSM,\langle\mathsf C,\mathsf J\rangle = \mathrm{NLSM},

⟨G,J⟩=Born ⁣− ⁣Infeld,\langle\mathsf G,\mathsf J\rangle = \mathrm{Born\!-\!Infeld},

⟨J−,J+⟩=special Galileon.\langle\mathsf J^-,\mathsf J^+\rangle = \mathrm{special\ Galileon}.

These pairings close the J\mathsf J row at cohomology level. A complete monoidal scalar normal-cone representative still requires the dependent-face coefficient lift; no additional cohomology class is required, but additional chain-level specialization data is.

Epistemic boundary

Established:

  1. representation-independent scalar-derived period covector;
  2. canonical derived index raising;
  3. equality of the resulting CHY class with [(Pf⁡′A)2][(\operatorname{Pf}'A)^2];
  4. factorization in the Pochhammer/Cousin complex on the transverse occurrence-decorated subcomplex;
  5. nested-cut monoidality on normal-crossing/transverse channel strata;
  6. correct nearby-cycle channel quotient at resonance;
  7. agreement with reduced-Pfaffian degeneration;
  8. cohomology-level closure of the J\mathsf J row in the genus-zero three-generator table.

Not established:

  1. a complete occurrence-decorated scalar-to-Pochhammer chain map across dependent/nontransverse faces;
  2. factorization naturality of one global scalar-derived half-chain before pairing;
  3. equality of a preferred point-set chain or smooth form with the rational Pfaffian expression;
  4. uniqueness of the finite-α′\alpha' regulator lift as a string completion;
  5. a canonical dg inverse of the pairing outside the derived category;
  6. modular/all-topology completion of this surface half-object;
  7. the proposed adjunction between the scalar first jet and scalar-scaffold lowering operators.

Decision

Promote:

The rank-jump/Jordan primitive is an intrinsic cohomological half-object of the scalar master: its complete scalar-derived period vector and derived Verdier index raising identify it uniquely with [(Pf⁡′A)2][(\operatorname{Pf}'A)^2]. Its finite-nonresonant Pochhammer/Cousin lift and pre-pairing factorization are established on the transverse subcomplex; the complete chain-level statement awaits the nontransverse coefficient lift.

The immediate Nima frontier is again the strongest original one:

construct the loaded five-term Cousin identity on one route pentagon and its companion square, using the two saturated incidence/Čech resolutions of entry 72, and thereby complete—or falsify—the factorization-natural scalar half-chain before pairing.

Only after that closure should the lowering-operator adjunction return to the front of this branch.

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