In the mathematical field of knot theory, the Jones polynomial is a knot polynomial discovered by Vaughan Jones in 1983. Specifically, it is an invariant of an oriented knot or link given by a Laurent polynomial in the variable with integer coefficients.
First, we define the auxiliary polynomial (also known as the normalized bracket polynomial) , where w(L) denotes the writhe of L in its given diagram. The writhe of a diagram is the number of positive crossings (L+ in the figure below) minus the number of negative crossings (L-). The writhe is not a knot invariant.
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 under a type I Reidemeister move. The definition of the X polynomial given above is designed to nullify this change, since the writhe changes appropriately by +1 or -1 under type I moves.
Now make the substitution in X(L) to get the Jones polynomial V(L). This results in a Laurent polynomial with integer coefficients in the variable .
Jones' 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 of the braid group on n strands, Bn, into the Temperley-Lieb algebra TLn with coefficients in and . A standard braid generator gets sent to , where are the standard generators of the Temperley-Lieb algebra. It can be checked easily that this defines a representation.
Take the braid word obtained previously from L and compute where tr is the Markov trace. This gives , 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".
The definition of the Jones polynomial by the bracket makes it simple to check that for a knot K, the Jones polynomial of its mirror image is given by substitution of for t in V(K). Thus, an amphicheiral knot, a knot equivalent to its mirror image, has palindromic entries in its Jones polynomial.
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