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Bracket polynomial

From Wikipedia, the free encyclopedia

In the mathematical field of knot theory, the bracket polynomial (also known as the Kauffman bracket) is a polynomial invariant of framed links. Although it is not an invariant of knots or links (as it is not invariant under type I Reidemeister moves), a suitably "normalized" version yields the famous knot invariant called the Jones polynomial. The bracket polynomial plays an important role in unifying the Jones polynomial with other quantum invariants. In particular, Kauffman's interpretation of the Jones polynomial allows generalization to invariants of 3-manifolds.

The bracket polynomial was discovered by Louis Kauffman in 1987.

YouTube Encyclopedic

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  • Introduction to the Kauffman Bracket
  • Kauffman Bracket, Writhe, and Reidemeister Moves
  • Francis Bonahon at SUNY Binghamton: Character varieties of surfaces and Kauffman brackets

Transcription

Definition

The bracket polynomial of any (unoriented) link diagram , denoted , is a polynomial in the variable , characterized by the three rules:

  • , where is the standard diagram of the unknot
  • Kauffman bracket2.png

The pictures in the second rule represent brackets of the link diagrams which differ inside a disc as shown but are identical outside. The third rule means that adding a circle disjoint from the rest of the diagram multiplies the bracket of the remaining diagram by .

Further reading

  • Louis H. Kauffman, State models and the Jones polynomial. Topology 26 (1987), no. 3, 395--407. (introduces the bracket polynomial)

External links

This page was last edited on 7 May 2014, at 16:44.
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