ScalingStacks

Then the quantity

K⁡(D)=(−1)x⁡(D)​qy⁡(D)−2​x​(D)<D>K(D)=(-1)^{x(D)}q^{y(D)-2x(D)}<D> (21)

does not depend on the choice of a diagram DD of the oriented link LL and is an invariant of L.L. We denote this invariant by K⁡(L).K(L). Up to a simple normalization, K⁡(L)K(L) is the Kauffman bracket of link LL and equal to the Jones polynomial of L.L. The Kauffman bracket, f⁡[L],f[L], as defined in [Ka], is a Laurent polynomial in an indeterminate AA (this AA has no relation to the algebra AA in Section 2.2 of this paper). One easily sees that setting our qq to −A−2-A^{-2} and dividing by (−A2−A−2)(-A^{2}-A^{-2}) we get f⁡[L]f[L]:

K​(L)(q=−A−2)=(−A2−A−2)​f​[L]K(L)_{(q=-A^{-2})}=(-A^{2}-A^{-2})f[L] (22)

In this paper we will call K⁡(L)K(L) the scaled Kauffman bracket.

Original mathematics by the credited authors. Source collection and HTML conversion remain in progress.

Mikhail Khovanov

Original source: arXiv:math/9908171v2