Definition by the bracketSuppose we have an oriented link L, given as a knot diagram. We will define the Jones polynomial, V(L), using Kauffman's bracket polynomial, which we denote by First, we define the auxiliary polynomial (also known as the normalized bracket polynomial) X(L) is a knot invariant since it is invariant under changes of the diagram of L by the three Reidemeister moves. Invariance under type II and III Reidemeister moves follows from invariance of the bracket under those moves. The bracket polynomial is known to change by multiplication by Now make the substitution A = t − 1 / 4 in X(L) to get the Jones polynomial V(L). This results in a Laurent polynomial with integer coefficients in the variable t1 / 2. Definition by braid representationJones' original formulation of his polynomial came from his study of operator algebras. In Jones' approach, it resulted from a kind of "trace" of a particular braid representation into an algebra which originally arose while studying certain models, e.g. the Potts model, in statistical mechanics. Let a link L be given. A theorem of Alexander's states that it is the trace closure of a braid, say with n strands. Now define a representation ρ of the braid group on n strands, Bn, into the Temperley-Lieb algebra TLn with coefficients in Take the braid word σ obtained previously from L and compute δn − 1trρ(σ) where tr is the Markov trace. This gives < L > , where < > is the bracket polynomial. This can be seen by considering, as Kauffman did, the Temperley-Lieb algebra as a particular diagram algebra. An advantage of this approach is that one can pick similar representations into other algebras, such as the R-matrix representations, leading to "generalized Jones invariants". PropertiesThe Jones polynomial is characterized by the fact that it takes the value 1 on any diagram of the unknot and satisfies the following skein relation: where L + , L − , and L0 are oriented link diagrams that are identical except in a small region where they differ by crossing change or smoothing as in the figure below: The definition of the Jones polynomial by the bracket makes it simple to show that for a knot K, the Jones polynomial of its mirror image is given by substitution of t − 1 for t in V(K). Thus, an amphicheiral knot, a knot equivalent to its mirror image, has palindromic entries in its Jones polynomial. See the page on skein relation for an example of a computation using these relations. Link with Chern-Simons theoryAs first shown by Edward Witten, the Jones polynomial of a given knot γ, can be obtained by considering Chern-Simons theory on the three-sphere with gauge group SU(2), and computing the vacuum expectation value of a Wilson loop WF(γ), associated to γ, and the fundamental representation F of SU(2). Open problems
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