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TauCeti.KnotTheory.Markov.TristramLevine

The Tristram–Levine signature of a closed braid #

Seifert's algorithm turns a braid word w into a Seifert surface for its closure, whose Seifert matrix in a basis of loops is TauCeti.BraidWord.seifertMatrix w. This file shows that the Tristram–Levine signatures σ_ω of that matrix depend only on the Markov equivalence class of the braid w represents, so they are invariants of the oriented link obtained by closing it (by Markov's theorem, which is not formalized here).

Two words representing the same braid have the same signatures (TauCeti.BraidWord.tristramLevineSignature_seifertMatrix_eq_of_toBraid_eq), since Artin relations and free cancellation change the matrix by a congruence, an elementary enlargement, or a zero row and column. This defines TauCeti.MarkovBraid.tristramLevineSignature on braids. Since inserting σᵢ σᵢ⁻¹ on every unused level gives a word whose canonical surface is connected, the value is the signature of a connected Seifert surface of the closure. Conjugation c b c⁻¹ is a cyclic rotation of a word followed by a free cancellation (TauCeti.BraidWord.tristramLevineSignature_seifertMatrix_rotate), and stabilization only relabels the loops (TauCeti.BraidWord.tristramLevineSignature_seifertMatrix_stabilize), so the signature is constant on Markov equivalence classes (TauCeti.MarkovEquiv.tristramLevineSignature_eq).

Unlike the Alexander polynomial, which is symmetric under t ↦ t⁻¹, the signature can tell a knot from its mirror image: mirroring negates it, so it separates the two whenever it is nonzero. The braid σ₀³ closes to the right-handed trefoil, of signature -2, and σ₀⁻³ to the left-handed one, of signature 2, so the two braids are not Markov equivalent (TauCeti.not_markovEquiv_sigma_pow_three_sigma_inv_pow_three). Informally, by Markov's theorem, the trefoil is not isotopic to its mirror image.

Main definitions #

Main results #

References #

The Tristram–Levine signature at ω of the closure of a braid: the signature of the Hermitian form (1 - ω) V + (1 - conj ω) Vᵀ, where V is the Seifert matrix of the canonical Seifert surface of the closure of a word representing the braid. It does not depend on the word (TauCeti.MarkovBraid.tristramLevineSignature_eq_of_toBraid_eq).

Instances For

    The Tristram–Levine signature of a braid is computed by any word representing it.

    @[simp]

    The Tristram–Levine signature of the braid represented by a word is that of the word's Seifert matrix.

    A single Markov move does not change the Tristram–Levine signature.

    The Tristram–Levine signature is a Markov invariant. Markov-equivalent braids have the same Tristram–Levine signature at every ω; by Markov's theorem, it is an invariant of the oriented link obtained by closing the braid.

    The right- and left-handed trefoils #

    The right-handed trefoil has signature -2. The braid σ₀³ closes to the right-handed trefoil, and its Seifert matrix has classical signature -2.

    The left-handed trefoil has signature 2. The braid σ₀⁻³ closes to the left-handed trefoil, the mirror image of the closure of σ₀³.

    theorem TauCeti.not_markovEquiv_sigma_pow_three_sigma_inv_pow_three :
    ¬MarkovEquiv { predStrands := 1, braid := BraidGroup.sigma 0 ^ 3 } { predStrands := 1, braid := (BraidGroup.sigma 0)⁻¹ ^ 3 }

    The trefoil braid is not Markov equivalent to its mirror image. The braids σ₀³ and σ₀⁻³, whose closures are the right- and left-handed trefoils, are not Markov equivalent: their Tristram–Levine signatures at ω = -1 are -2 and 2. The Alexander polynomial cannot separate them, being the same for a knot and its mirror image. Informally, by Markov's theorem, the trefoil is chiral.