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 #
TauCeti.MarkovBraid.tristramLevineSignature β ω: the Tristram–Levine signature atωof the Seifert matrix of any braid word representingβ.
Main results #
TauCeti.MarkovBraid.tristramLevineSignature_eq_of_toBraid_eq: the signature of a braid is that of the Seifert matrix of any word representing it.TauCeti.IsMarkovMove.tristramLevineSignature_eqandTauCeti.MarkovEquiv.tristramLevineSignature_eq: the Tristram–Levine signature is a Markov invariant.TauCeti.MarkovBraid.tristramLevineSignature_sigma_pow_three_neg_oneandTauCeti.MarkovBraid.tristramLevineSignature_sigma_inv_pow_three_neg_one: the right- and left-handed trefoils have signatures-2and2.TauCeti.not_markovEquiv_sigma_pow_three_sigma_inv_pow_three: soσ₀³andσ₀⁻³are not Markov equivalent.
References #
- W. B. R. Lickorish, An Introduction to Knot Theory, Springer GTM 175 (1997), Chapter 6 (Seifert matrices) and Chapter 8 (the signature, and S-equivalence).
- A. G. Tristram, Some cobordism invariants for links, Proc. Cambridge Philos. Soc. 66 (1969), 251–264.
- J. Birman, Braids, Links, and Mapping Class Groups, Annals of Mathematics Studies 82 (1974), Chapter 2 (Markov's theorem).
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.
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.
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.