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LemmaStatement: Literature-sourcedProof: AI-adaptedPipeline-generatedverified 2026-10-22 (gpt-6.1-sol)
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Marked integral odd Reidemeister I and II contractions

Statement

For a finite planar odd resolution cube with the prescribed full face signs, a Reidemeister I or II move supported away from the marked point induces a normalized bigraded chain homotopy equivalence over the right ring A=Z[X]/(X2). The equivalence, inverse and contraction are finite integer matrices in exterior quotients, exterior products, and projections to the two coefficients of a small-circle generator. Their reductions modulo two are the corresponding even Khovanov cancellation maps. The result holds for every exterior closure of the move disk and every orientation of its strands, and is choice-free.

Facts & Assumptions

Given: A based diagram, a move disk missing the mark, and the finite exterior cubes at the two sides.

[F1]

Odd edge maps are the exterior quotient and the split difference wedged on the left; the marked action is wedged on the right (Odd Khovanov–Bar–Natan–LEO triple).

[F2]

The prescribed face signs exist, and changing their realization gives a grading-preserving vertex-sign module isomorphism (Oriented odd-cube face parity and constructive edge signs).

Proof

Given: The hypotheses of the Statement. Exterior crossings are ordered first, and their vertex is denoted v.

1.1givenalgebraconstruct

A cancellation identity over any ring. Suppose a cochain differential d on M=A⊕B⊕R has a degree-one block b:A→B which is an isomorphism. Set h∣B=b−1 and h∣A⊕R=0. Then h2=0 and hdh=h. Consequently E=1−dh−hd is a projection commuting with d: expansion using d2=h2=0 and hdh=h gives E2=E and dE=Ed. Writing j:R→M and q:M→R for the direct-sum maps, set i=Ej=j−hdj, p=qE=q−qdh, and dR=q(d−dhd)j. The A-coordinate of a vector in im⁡E is minus hd of its R-coordinate, and its B-coordinate is zero; hence q:im⁡E→R and Ej are inverse. Thus pi=1, ip=E, di=idR, pd=dRp, and 1−ip=dh+hd. These identities also give dR2=0. If the blocks and their inverse are right-module maps, so are all these maps. This calculation applies to entire finite exterior cubes at once; their differentials are included in d, rather than omitted as spectators.

1.2F1F2algebraconstruct

The RII four-state model. Call the straight matching I and the cup-cap matching U. Rotate the disk and order the crossing whose smoothing pair is (I,U) first, followed by the crossing whose smoothing pair is (U,I). This order refers to the geometric smoothings; for either orientation of the two strands the pair contains one oriented positive and one oriented negative crossing. The local states 00,01,10,11 are U,I,U⊔z,U. In state 10 label the circle through the upper arc a, the small circle z, and the circle through the lower arc c; the exterior closure may identify a and c. These labels therefore denote actual generators, with that equality imposed when applicable. At 00→10 the map is the split (a−z)∧(−) after choosing its lift; at 10→11 the quotient identifies z with c. Each edge has its prescribed sign, which is ±1 and may depend on v. In 10 set Y=z−c and write L=ΛW, K=Y∧ΛW, where W is the circle group of U. The quotient 10→11 is the identity on L and zero on K. The K-coefficient of 00→10 is minus the identity, because a−z=(a−c)−Y. This remains true when a=c. Thus both indicated blocks are invertible right-module blocks for every exterior closure.

2.1F1F2step 1.1algebraconstruct

The merge curl. Write Wv for the old circle group and cv for the circle through the curl's continuing arc. The two local states are Λ(Wv⊕Zz) and ΛWv, with merge quotient m(z)=m(cv)=cv. Put Y=z−cv and decompose the first state as Lv⊕Kv, where Lv=ΛWv and Kv=Y∧ΛWv. The merge is the identity Lv→ΛWv and kills Kv. External edges preserve both summands. Indeed a merge takes Y to its new Y, while a split takes Y to the new Y up to a multiple of its own split difference; that extra term vanishes when wedged with the same difference. On L the external maps are the old maps. On K, identifying Y∧w with w negates each external split and leaves each merge unchanged. Put σ(v)=(k(v)−k(0)+∣v∣)/2. It is an integer, unchanged by a merge and increased by one by a split. Thus w↦(−1)σ(v)Y∧w identifies K with the old complex. The other two summands cancel by step 1.1, using the signed merge pivot and its inverse. With the ordinary cube ordering its pivot coefficient can be taken (−1)∣v∣. The normalization makes the survivor's cohomological and quantum degrees those of the old diagram: the extra small circle and extra exterior generator change the local quantum degree by −1, cancelling the positive-curl shift +1.

2.2step 1.1step 1.2algebraconstruct

The two RII cancellations. First cancel L10→U11 by step 1.1. Its inverse is the signed inclusion using no z. The correction −dhd does not alter the 00→K10 block, since external edges preserve L and the local outgoing arrow from L lands only in 11. That block is still the signed minus identity, so cancel U00→K10. The survivor is I01. Its exterior differential is unchanged: after the first cancellation no differential from I01 enters K, since its only local outgoing edge was to the cancelled 11 and the correction factors through L, which has no K-component. Consequently the second cancellation contributes no correction on I01. The local height is one, the pair adds one negative and one positive crossing, and hence the homological shift is 1−1=0 and the quantum shift is 1+(1−2)=0. This proves the normalized equivalence.

3.1F1F2step 1.1step 2.1algebraconstruct

The split curl. Here the local arrow is ΛWv→Λ(Wv⊕Zz), w↦Y∧w, with either overall sign allowed. Use the same decomposition L⊕K. The split is an isomorphism onto K; L survives. Choose the crossing-edge coefficient (−1)∣v∣+σ(v) when the external edges have their old coefficients. Across an external merge this coefficient changes sign, and across a split it is unchanged. Since the unsigned curl split commutes with the former and anticommutes with the latter, every mixed square anticommutes. Cancel its isomorphism onto K by step 1.1. The surviving L has its old differential and right action. It is at local height one; the negative crossing increases n− by one, so its normalized cohomological degree is unchanged. Its additional circle contributes quantum degree +1, its local height contributes +1, and the negative crossing contributes −2, again giving shift zero. The formulas include both directions of the move, since the inclusion and projection are homotopy inverses.

4.1F1F2step 1.1step 3.1step 2.2algebra∎

Module maps, signs and reduction. The mark is outside the disk, so it is never the small circle z. In the displayed decompositions a right multiplication appends an old generator. Coefficient projections in z and Y=z−c, the inclusions, and multiplication by a left split difference therefore commute with that right action. All pivots, their signed inverses and the maps in step 1.1 are module-linear. Different admissible edge signs are accommodated by [F2]. Reversing a saddle arrow negates its split map and is absorbed in that edge coefficient; changing strand orientations changes only the normalized crossing shifts, already checked for R1 and RII. Rotations simply relabel the generators and disk ports. Modulo two all displayed signs become one, exterior products become commuting square-zero circle labels, and z−c becomes z+c. Merge, split, inclusion, coefficient projection and the formula d−dhd reduce to precisely the even cancellation operations. Thus the maps, inverses and homotopies have the asserted comparison, for every closure and orientation.

Depends on

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Sources