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Connected sums and prime decomposition — Examples and Counterexamples
1 · Prerequisites
- Abelian Categories
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2 · Logical flowchart
3 · Definitions, theorems and proofs
None yet.
4 · Examples, counterexamples and false statements
Connected-sum genus and ribbon examples
Example
Assume full AC. Let be the standard right-handed trefoil, let be its image under a fixed orientation-reversing reflection of , and let denote reversal of that image's knot orientation. Then and . The knot bounds a smooth ribbon disk in , meaning a smooth properly embedded disk whose radial-height function has no interior local maxima; in particular it bounds a smooth properly embedded disk and is smoothly slice.
Example references
Facts & Assumptions
Given: Full AC, the standard right-handed trefoil, its reverse mirror, and the stated connected-sum operations.
The trefoil genus is exactly . (The right trefoil has genus one)
Genus is additive under connected sum. (Knot genus is additive under connected sum)
Mirroring and reversing orientation preserve genus. (Knot genus is invariant under mirroring and reversal)
The trefoil sum with its reverse mirror bounds a smooth ribbon disk. (The trefoil sum with its reverse mirror is ribbon)
Full AC is the choice-function axiom. (The Axiom of Choice)
Full AC implies AC. (AC implies DC implies countable choice)
The ribbon convention excludes interior radial maxima; index-zero minima and index-one saddles are allowed.
Verification
Given: Full AC and the two connected sums in the statement.
By [F1], , and by [F3], . Full AC implies the AC hypothesis of [F2] by [A2], so additivity gives and .
By [F4], bounds a smooth ribbon disk. A ribbon disk is in particular a smooth properly embedded disk, so the knot is smoothly slice. The explicit doubled-arc disk has no interior radial maxima, as required by the stated convention.
The Alexander polynomial does not determine the prime knot summands
Statement refuted
Assume the full Axiom of Choice. For an oriented Seifert surface with boundary and ordered basis of , let be the Seifert matrix with entries . Here is the integer linking number of disjoint oriented cycles in , and is a small push-off in the positive normal direction, chosen so that the positive normal followed by the oriented basis of gives the orientation of . Use the standard knot-invariant conventions up to units and , where the matrix sign is the number of positive eigenvalues minus the number of negative eigenvalues; independence of the chosen surface and basis is part of the Seifert-form invariance theorems. Let be the standard right-handed trefoil, let be its image under a fixed orientation-reversing reflection of , and let be that image with reversed knot orientation. Define and . Then , and while . The oriented prime-factor multisets of and are different. Thus equality of Alexander polynomials does not determine the prime knot summands.
Statement references
Facts & Assumptions
Given: The full AC, knots , positive-push and invariant conventions of the original Statement.
Full AC implies countable choice, as required by the prime and smooth knot suppliers. The Axiom of Choice, AC implies DC implies countable choice
The actual right-handed trefoil bounds the standard positive two-Hopf-band plumbing, whose positive-push matrix in its ordered core basis is . The handedness and negative diagonal signs are the established geometric convention, not the differently labeled positive matrix in the source-specific KT06 example. A positive Hopf plumbing gives the trefoil Seifert matrix ↗, The canonical positive three-crossing braid has the negative trefoil form
For every knot Seifert surface with the same positive normal and positive-meridian convention, . The actual boundary connected-sum surface has block matrix : the old bases lie in separated balls and both cross-linking blocks vanish. The Seifert determinant is the knot Alexander polynomial ↗, The knot Alexander polynomial multiplies under connected sum ↗, Proof2.1–4.1.
At every nonroot point , the signature of is an oriented knot invariant independent of surface and basis. The full knot-surface S-equivalence and stabilization proofs now establish this actual interface. Levine–Tristram Hermitian form and signature ↗, Seifert matrices of a knot are S-equivalent ↗, Seifert stabilization preserves the Levine–Tristram signature ↗
The right trefoil is prime, reflection preserves nontriviality and primality, and the oriented prime decomposition is unique up to ordering and insertion/deletion of unknot factors. The right trefoil is prime, Mirroring preserves primeness of an oriented knot, Existence and uniqueness of prime decomposition for oriented knots, Oriented connected sum and prime knot
Refutation
Given: The actual right-trefoil matrix in [F1], with all the Statement's knot and orientation conventions.
By [F1] and [F2], For use the reflected spanning surface with its surface orientation reversed, so its boundary is the reversed reflected knot. Its positive normal is the reflected original positive normal: ambient reflection and surface reversal each negate the orientation, so their effects cancel in the normal-first convention. Reflection negates linking. The transported homology basis on this actual surface consequently has matrix . Its determinant is , since the matrix size is two. The two determinants evaluate to at , so this parameter is nonroot and [F3] applies directly, with no root-average ambiguity.
By [F2], the actual boundary connected-sum surfaces of and have matrices and . Their block determinants both equal , proving the two Alexander-polynomial identities up to units. Also Its eigenvalues on the vectors and are and , respectively. Thus and . The corresponding block forms give and . These are actual knot-invariant values by [F3], since the sum polynomials at equal . In particular as stated.
By [F4], and are nontrivial prime oriented knots. Reversal of knot orientation also preserves these properties: reverse both factors and the two local oriented arcs in any purported nontrivial connected-sum presentation of to obtain a nontrivial presentation of ; reversing again is the inverse operation, and the unknot remains the unknot. Thus is prime. The signatures in step2.1 show that and are distinct oriented knot types, since an oriented ambient isotopy would preserve [F3]'s signature. Therefore the displayed two-prime decompositions have respective multisets and , which are different. By [F4]'s actual oriented Schubert uniqueness they are the prime-factor multisets of and , independent of a chosen decomposition. Together with their equal Alexander polynomials, this proves the entire original refutation. No planned matrix interface or conditional prime/invariant premise remains.
Sources
Oriented connected sum and prime knot
Existence and uniqueness of prime decomposition for oriented knots
Seifert pairing and matrix of an oriented knot ↗
The Seifert determinant is the knot Alexander polynomial ↗
The knot Alexander polynomial multiplies under connected sum ↗
Levine–Tristram Hermitian form and signature ↗
Seifert stabilization preserves the Levine–Tristram signature ↗