For a nonempty unoriented link diagram , the reduced Kauffman bracket is the Laurent polynomialThe sum runs over bracket smoothing states; and count the two smoothing choices, and counts the resulting circles. Thus one circle has bracket one, each additional disjoint circle multiplies by , and a crossing expands with weights and . The smoothing convention is fixed by marking the two sectors swept out when the overpassing line turns counterclockwise toward the underpassing line as the sectors.[ref]
State models and the Jones polynomial by Louis H. Kauffman. Definition 2.1 and Figure 2, pages 396–397
The Kauffman bracket is invariant under the second and third Reidemeister moves. A positive or negative curl instead multiplies it by or , respectively. Correcting this factor by the writhe of a link diagram produces the Jones polynomial. For two crossing-free circles, the bracket is simply .
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