Vector-valued differential form: Difference between revisions

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Corrected the product rule for the covariant exterior derivative
en>TakuyaMurata
 
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In the [[mathematics|mathematical]] field of [[knot theory]], the '''bracket polynomial''' (also known as the '''Kauffman bracket''') is a [[polynomial]] invariant of [[framed link]]s. Although it is not an invariant of knots or links (as it is not invariant under type I [[Reidemeister move]]s), 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 invariant]]s.  In particular, Kauffman's interpretation of the Jones polynomial allows generalization to invariants of [[3-manifold]]s. 
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The bracket polynomial was discovered by [[Louis Kauffman]] in 1987.
 
==Definition==
The bracket polynomial of any (unoriented) link diagram ''L'', denoted <''L''>, is a polynomial in the variable <math>A</math>, characterized by the three rules:
 
*  <O> = 1, where O is the standard diagram of the unknot
[[Image:kauffman_bracket2.png|275px]]
* <math> \langle O \cup L \rangle = (-A^2 - A^{-2}) \langle L \rangle </math>
 
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 ''-A<sup>2</sup> - A<sup>-2</sup>''.
 
==Further reading==
*Louis H. Kauffman, ''State models and the Jones polynomial.'' Topology 26 (1987), no. 3, 395--407.  (introduces the bracket polynomial)
 
==External links==
*{{MathWorld|BracketPolynomial|Bracket Polynomial}}
 
{{Knot theory}}
 
[[Category:Knot theory]]
[[Category:Polynomials]]
 
{{knottheory-stub}}

Latest revision as of 02:26, 18 December 2014

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