CHERN-SIMONS THEORY AND LINK INVARIANTS! Dung Nguyen! U of Chicago!
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1 CHERN-SIMONS THEORY AND LINK INVARIANTS! Dung Nguyen! U of Chicago!
2 Content! Introduction to Knot, Link and Jones Polynomial! Surgery theory! Axioms of Topological Quantum Field Theory! Wilson loopsʼ expectation value!
3 Knot and Link? Knot is a smooth non-intersecting closed curved in threemanifold. Oriented closed curves are oriented knots.!
4 With given knot, we associate a knot diagram obtained by projecting the knot on to a plane.!
5 Link is a collection of non-intersect loops (knots). A knot then is a single component link, we also have link diagram as the projection of a link on plane.!
6 Remarks: A link is well-determined by one of its diagram.! One knot (link) can have different knot (link) diagrams depending on how we map the knot on the plane.! We have following diagram for right-hand trefoil knot!
7 Reidemeister theorem (1926):! Up to orientation preserving diffeomorphism of the plane, two diagrams of a link can be related by a finite sequence of (local) Reidemeister moves!!
8 Crossing change is a local modification of the type! Note that it is not a Reidemeister move.! Theorem: Any link can be unknotted by a finite number of crossing changes.!!
9 Link invariant! Link invariant is a map from set of links to and other set (In the case of Jones polynomial the other set are polynomials).! Such a map can be defined as function of diagrams that is invariant under Reidemeister moves.! Positive crossing in a diagram is the crossing! Negative crossing in a diagram is the crossing!
10 Jones Polynomial and link invariant! Let D be an unoriented link diagram. A crossing of D can be removed in two different ways.! Left hand (L):! Right hand (R):!
11 Let C(D) be the set of crossing of D and be a map from C(D) to, then will denote the diagram by remove crossing x in left-hand way if and in the right-hand way if.! Is nothing but a collection of circles embedded in the plane.! We define Kauffman bracket <D> as! With! Where A is a variable.!
12 Example
13 Properties of Kauffman bracket!! In the following properties, the related brackets of diagrams are identical everywhere except where they are drawn!
14 Define of an oriented link diagram D is the number of positive crossing minus the number of negative ones.! Jones polynomial V(L) of an oriented link L is the polynomial from an oriented diagram D of L by! V is invariant of oriented links. It is unique invariant of oriented links that satisfies! We can prove (2) from property 4 th of Kauffman bracket.!
15 Some important remarks on Jones polynomial:! When we specify t, the value V(L) of each oriented link is unique. Jones polynomial is Link invriant.! From the skien relations, and previous theorem, we can calculate Jones polynomial for any link with enough patient.! The idea is any link can be unknotted by finite crossing changes, and the V(L) of a n-component trivial link is trivial!
16 Surgery theory in 3-malnifolds! Heegard splitting and gluing:! Every compact orientable 3-manifold can be presented as gluing 2 handle-bodies with the same genus along their common boundaries.! Gluing is merging 2 manifolds with boundary with a diffeomorphism map between their boundaries (we will see in the examples).! f : M M 1 2
17 Letʼs see the gluing of 2 solid tori!
18 If we gluing 2 tori after S-dual when we map contractible circle of one torus to the other meridian circle.! Letʼs see how does it happen! D 3 We can glue 2 on their boundaries to get! S 3
19 The most important surgeries are surgery along a link or surgery along a knot.! We remove the tubular neighborhood of link L from and reglue it back after a diffeomorphism.! The p/q ( with p and q are coprime) surgery is the surgery with the specific diffeomorphism that pa+qb circle becomes contractible circle ( a circle)! S 3
20 The surgery a long a knot which is the group of mapping torus to it self (SL(2,Z) group) can be decomposed in to S transformation and T transformation, the matrix form of the transformations are! And we also have! Which map pa+b circle into b circle. It is also called Dehn twist, we open the solid torus along a-circle and reglue after p twists.! And S transformation exchanges the one-circles of the torus.! Why we care about surgery theory?!
21 Chern-Simons theory as TFT! Consider C-S action! The C-S action is metric independent! A is the G-gauge connection on principle bundle on base space M.! k is integer named level ( inverse of coupling constant)! Integrate out! A t ( we have flat gauge curvature)!
22 Chern-Simons theory is an example of topological quantum field theory.! TQFT has set of operators ( observables) whose correlation functions do not depend on metric of base space M.! In Chern-Simons theory, the operators are Wilson loop operators! It is the Wilson loop along oriented knot K in representation R of group G.!
23 Consider link L with L knot component, we can in principle calculate normalized correlation function! The complicated link can be derive from simple knots by using surgery.!
24 Axioms of TQFT ( specify for C-S)! Let be a 3-manifold with boundary given by Riemann surface, we can insert operator as product of Wilson loops.! We consider the case that Wilson loops do not intersect boundary of M.! The path integral over M gives wave function is a function of value of field on!
25 Associated to Riemann surface we have Hilbert surface which obtain by canonical quantization of C-S theory on (Hilbert space axiom)! We can consider two 3-manifolds and sharing common boundary. We glue and by homeomorphism! Path integral over is state!
26 In gluing process share the same boundary but with opposite orientation, so it Hilbert space is the dual space (Orientation axiom). The path integral over gives us a state.! The homeomorphism will be represented as a unitary operator! Finally, partition function on manifold M is! Where!
27 Wilson loop expectation value on S 3! We consider the group is SU(2) We know that a S 3 manifold can be consider as a gluing of 2 solid tori! = T 2 The common boundary is We denote the state! ",k in the Hilbert space can be described by placing a Wilson line inside the torus along b-circle transform in the representation of weight! / 2. With! = 0 (trivial representation) we do not insert any Wilson loop.
28 Using canonical quantization of Chern-Simons theory on the torus T 2! R, in the case of group SU(2), we can derive metric elements ( The calculation can do in geometrical quantization and also in conformal field theory )! S 2 π ( a+ 1)( b+ 1) = ψ Sψ = sin k+ 2 k+ 2 ab a, k b, k In which S is the S-transformation that we mentioned before.! After gluing 2 tori using S-transformation, we have S 3 manifold with a Hopf link including 2 Wilson loop with in different representations.!
29 Further more, we also can derive that the transformation T just gives state a phase! T ψ 2πi 2πic C2 ( γ ) k γ, k = e ψγ, k In which C 2 is quadratic Casimir of the representation and c is the central charge of WZW model, in SU(2) we have! k c = k + 2
30 From that we have some expectation value of Wilson loop in S 3! The partition function as gluing 2 solid tori without any Wilson loop.! Expectation value of a Wilson loop in representation with spin 1/2! Expectation value of a Hopf link with 2 spin ½ Wilson loop!
31 As the link gets more complicated, the direct computation becomes harder. Instead, we have the skein relation of a link in representation spin=1/2!! Using surgery operators we also can derive the relation! Jones polynomial with q=t!!
32 Conclusion We had some fun with links and knots Surgery is not always hurt Jones polynomials make the calculations easy
33 Appendix Heegard splitting
34 Heegard splitting! The idea behind:! Every compact orientable 3-manifold has a finite tetrahedralization ( splitting into tetrahedrons).! The one-skeleton is the union of all vertices and edges of tetrahedralization, if we Hthicken 1 it up, we has a handle body within 3-manifold!
35 We also have the dual graph of the tetrahedralization, it is also handle body with the same genus as the tetrahedralization, if we thicken both of them enough, they will fill up the 3-manifold M and share the same boundary as gluing map.! H 2 The gluing that weʼve seen is Heegard splitting of manifold M into and H.! H1 2
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