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Advances in Knot Polynomials 21 October 2016 Advances in Knot Polynomials 21 October 2016 1 / 49 ABSTRACT Review of achievements and problems in the theory of colored knot polynomials. Accent is on the current mystery around the differential


  1. Advances in Knot Polynomials 21 October 2016 Advances in Knot Polynomials 21 October 2016 1 / 49

  2. ABSTRACT Review of achievements and problems in the theory of colored knot polynomials. Accent is on the current mystery around the differential expansion and Racah matrices (6j-symbols) in rectangular representations. Advances in Knot Polynomials 21 October 2016 2 / 49

  3. J.W.Alexander, Trans.Amer.Math.Soc. 30 (2) (1928) 275-306 V.F.R.Jones, Invent.Math. 72 (1983) 1 P.Freyd, D.Yetter, J.Hoste, W.B.R.Lickorish, K.Millet, A.Ocneanu, Bull. AMS. 12 (1985) 239 J.H.Przytycki and K.P.Traczyk, Kobe J. Math. 4 (1987) 115-139 L.Kauffman,Topology 26 (1987) 395 Advances in Knot Polynomials 21 October 2016 3 / 49

  4. Colored HOMFLY polynomial: � � � H K R ( A , q ) = Tr R P exp A K average with CS action with the gauge group G = SL ( N ) : � � � A d A + 2 3 A 3 κ Tr M 2 π i q = exp κ + N A = q N Advances in Knot Polynomials 21 October 2016 4 / 49

  5. HOMFLY are exactly-calculable non-perturbative averages in gauge QFT Advances in Knot Polynomials 21 October 2016 5 / 49

  6. For simply-connected M ( R 3 or S 3 ): Calculation of HOMFLY Properties of HOMFLY Generalizations of HOMFLY Relations to other theories Other M HOMFLY for virtual knots Advances in Knot Polynomials 21 October 2016 6 / 49

  7. A.Mironov A.Anokhina, S.Arthamonov, V.Dolotin, P.Dunin-Barkovski, D.Galakhov, H.Itoyama, Ya.Kononov, D.Melnikov, An.Morozov, P.Ramadevi, Vivek Singh, Sh.Shakirov, A.Sleptsov, A.Smirnov Advances in Knot Polynomials 21 October 2016 7 / 49

  8. Calculation of HOMFLY Modernized Reshetikhin-Turaev calculus Paths in representation graphs Eigenvalue hypothesis Arborescent knots – new effective theory Fingered braids – the most efficient tool at the moment Evolution/family method . . . Advances in Knot Polynomials 21 October 2016 8 / 49

  9. other 2d 3d higher d Seifert surfaces CFT ✟✟✟✟ ✯ ❅ ■ ✻ � ✒ ❅ � CS ❄ projection to 2d lattice theory on arbitrary graphs � ❅ ✠ � ❅ ❘ algebra geometry RT KhR hypercube Advances in Knot Polynomials 21 October 2016 9 / 49

  10. RT calculus traditional ✻ ✻ tr q ρ . . . R ± 1 ✻ 34 R ± 1 modern 23 ✻ � Q D Q · Tr W Q . . . R ± 1 12 ✻ R k l † R Q 23 = U Q 23 R Q 12 U Q 23 i j � � R Q 12 = diag ǫ Y · q κ Y ✻ R R ⊗ R ⊗ R ⊗ R = ⊕ Q ⊗ W Q ✻ ✻ � �� � R R ⊕ Y Advances in Knot Polynomials 21 October 2016 10 / 49

  11. Fundamental representation R = � : R − R − 1 = q − q − 1 skein relations paths in representation tree Advances in Knot Polynomials 21 October 2016 11 / 49

  12. Other representations R : cabling method eigenvalue hypothesis tree calculus – under construction not just braids Advances in Knot Polynomials 21 October 2016 12 / 49

  13. BRAID CALCULUS Needed is entire collection of mixing matrices For 3 strands needed are only Racah matrices S ( Q ) Y ′ Y ′′ � � � � ( R ⊗ R ) ⊗ R − → Q − → R ⊗ ( R ⊗ R ) − → Q � �� � � �� � Y ′ Y ′′ but "inclusive": for all Q ∈ R ⊗ 3 This is realistic, but too few knots are 3-strand Advances in Knot Polynomials 21 October 2016 13 / 49

  14. ARBORESCENT KNOTS/LINKS made from fingers, propagators and vertices Advances in Knot Polynomials 21 October 2016 14 / 49

  15. ARBORESCENT (double-fat) KNOTS/LINKS made from fingers, propagators and vertices Advances in Knot Polynomials 21 October 2016 15 / 49

  16. Advances in Knot Polynomials 21 October 2016 16 / 49

  17. Needed are just two "exclusive" Racah matrices � � � � ¯ ( R ⊗ ¯ R ⊗ (¯ S : R ) ⊗ R − → R − → R ⊗ R ) − → R and � � � � (¯ ¯ S : R ⊗ R ) ⊗ R − → R − → R ⊗ ( R ⊗ R ) − → R Advances in Knot Polynomials 21 October 2016 17 / 49

  18. T ¯ ¯ S ¯ T = ST − 1 S † T and ¯ T are diagonal matrices Advances in Knot Polynomials 21 October 2016 18 / 49

  19. FINGERED BRAIDS ✲ ✲ ✲ ✲ ✲ ✲ n 1 n 2 n 4 n 6 ✲ ✲ ✲ ✲ ✲ ✲ ✲ n 3 n 5 n 7 ✲ ✲ ✲ ✲ ✛ Advances in Knot Polynomials 21 October 2016 19 / 49

  20. FINGERED BRAIDS allow to handle more complicated knots by using less strands Three-strand fingered braids are already quite rich but even for them calculus is still hard Advances in Knot Polynomials 21 October 2016 20 / 49

  21. side stories: The structure of the space of knots Effective gauge field theory for arborescent knots Gauge invariance, vertices and loops Rectangular and non-rectangular representations Advances in Knot Polynomials 21 October 2016 21 / 49

  22. States: ✻ ✻ ✻ ✻ ✻ ✻ ❄ ❄ ❄ ❄ ❄❄ σ ϕ φ and conjugates: ✻ ✻ ✻ ✻ ✻ ✻ ❄ ❄ ❄ ❄ ❄ ❄ σ ∗ ϕ ∗ φ ∗ Each of them carries indices σ AB − → σ X αβ with the gauge group acting by two orthogonal matrices A and B : � σ X ,α,β − → A αα ′ B ββ ′ σ X ,α ′ β ′ α ′ β ′ Advances in Knot Polynomials 21 October 2016 22 / 49

  23. Quadratic terms in the Lagrangian are: "local"ones ϕ X ¯ σ X T n X σ X = σ X ,αβ T n T 2 n X ,αα ′ σ X ,α ′ β X ϕ X , φ X ¯ ϕ X ¯ φ X ¯ T 2 n T 2 n − 1 T 2 n X φ X , φ X , X ϕ X X plus conjugates, "non-local"ones X S † X ¯ σ ∗ φ ∗ ϕ ∗ XY φ Y , X S XY σ Y , S XY ϕ Y (note that there are no terms φ ∗ X φ Y ) Advances in Knot Polynomials 21 October 2016 23 / 49

  24. Topologically allowed vertices are Γ (1) ∼ σ 3 Γ (2) ∼ ϕ 3 Γ (3) ∼ φ 2 X , X , X ϕ X The problem is, however, to deal with the Greek indices in Γ α,β,γ Φ α,β Φ β,γ Φ γ,α . A naive anzatz like tr σ 3 X with the trace in Greek → A σ A † , but it indices would be good for a transformation law σ − violates σ − → A σ B with independent A and B . This means that at the representational level one can not get a gauge invariant description of our knot polynomials. If one calculates the Feynman diagram for some particular choice of S (in a particular gauge), the answer differs in other gauges so that there should be some "handy"compensational rule attached to the answer. Advances in Knot Polynomials 21 October 2016 24 / 49

  25. 2 n ❆ ✁ ☛ ❑ ❆ ✁ . . . ✁ ❆ ✁ ❆ ❯ ✕ ❍✟ 2 m . . . ✟ ✟❍ ❍❍ ❥ ✯ ✟ Advances in Knot Polynomials 21 October 2016 25 / 49

  26. EVOLUTION for twist and double braid knots � D µ D ν � H ( m , n ) S µν Λ 2 m ¯ µ Λ 2 n = ν R D R µ,ν ∈ R ⊗ ¯ R Advances in Knot Polynomials 21 October 2016 26 / 49

  27. Properties of HOMFLY Polynomiality and integralities Factorizations Equations Hurwitz integrability Vogel’s universality (unification of E 8 -sectors of all Lie algebras) Differential expansions . . . Advances in Knot Polynomials 21 October 2016 27 / 49

  28. . . . Advances in Knot Polynomials 21 October 2016 28 / 49

  29. DIFFERENTIAL EXPANSION Advances in Knot Polynomials 21 October 2016 29 / 49

  30. [1] = A 2 − q 2 + 1 − q − 2 + A − 2 H 4 1 = 1 + { Aq }{ A / q } A = q N { x } = x − 1 / x [ n ] = q n − q − n q − q − 1 = { q n } { q } Differentials { Aq n } ∼ [ N + n ] Advances in Knot Polynomials 21 October 2016 30 / 49

  31. H 4 1 [1] = 1 + { Aq }{ A / q } H 4 1 [2] = 1 + [2] { Aq 2 }{ A / q } + { Aq 3 }{ Aq 2 }{ A }{ A / q } H 4 1 [3] = 1 + [3] { Aq 3 }{ A / q } + [3] { Aq 4 }{ Aq 3 }{ A }{ A / q } + + { Aq 5 }{ Aq 4 }{ Aq 3 }{ Aq }{ A }{ A / q } . . . Advances in Knot Polynomials 21 October 2016 31 / 49

  32. Differential expansion Equations . . . Superpolynomials տ ↑ ր H 4 1 [1] = 1 + { Aq }{ A / q } H 4 1 [2] = 1 + [2] { Aq 2 }{ A / q } + { Aq 3 }{ Aq 2 }{ A }{ A / q } ւ ց Other representations Other knots [ r s ] = � H 4 1 λ ( r ) D λ ( s ) Z λ H K [1] = 1 + G K λ ∈ [ r s ] D ˜ [1] ( q , A ) { Aq }{ A / q } r | s Advances in Knot Polynomials 21 October 2016 32 / 49

  33. � { Aq r + a ′ ( � ) − l ′ ( � ) }{ Aq − s + a ′ ( � ) − l ′ ( � ) } Z λ r | s ( A , q ) = � ∈ λ l ′ ✻ ✛ ✲ a ′ a ❄ l { Aq − l ′ ( � )+ a ′ ( � ) } [ N − l ′ ( � ) + a ′ ( � )] � � D λ ( N ) = { q a ( � )+ l ( � )+1 } = [ a ( � ) + l ( � ) + 1] � ∈ λ � ∈ λ Advances in Knot Polynomials 21 October 2016 33 / 49

  34. Other knots: H K [1] = 1 + G K [1] ( q , A ) { Aq }{ A / q } H K [2] = 1 + [2] G K [1] ( q , A ) { Aq 2 }{ A / q } + G K [2] ( q , A ) { Aq 2 }{ A }{ A / q } only for defect zero : [1] ( q , A ) { Aq 2 }{ A / q } + F K 0 H K [2] = 1 + [2] F K [2] ( q , A ) { Aq 3 }{ Aq 2 }{ A }{ A / q } � � Al K defect = power q 2 - 1 [1] Advances in Knot Polynomials 21 October 2016 34 / 49

  35. Double braids have defect zero and very special F : � H ( m , n ) r | s · F ( m , n ) λ ( r ) · D λ ( s ) · Z λ = D ˜ ( q , A ) [ r s ] λ λ ⊂ [ r s ] Advances in Knot Polynomials 21 October 2016 35 / 49

  36. 2 n ❆ ✁ ☛ ❑ ❆ ✁ . . . ✁ ❆ ✁ ❆ ❯ ✕ ❍✟ 2 m . . . ✟ ✟❍ ❍❍ ❥ ✯ ✟ Advances in Knot Polynomials 21 October 2016 36 / 49

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