The Kauffman Polynomial: Difference between revisions
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(here <math>s</math> is a strand and <math>s_\pm</math> is the same strand with a <math>\pm</math> kink added) and |
(here <math>s</math> is a strand and <math>s_\pm</math> is the same strand with a <math>\pm</math> kink added) and |
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<center><math>L( |
<center><math>L(\backoverslash)+L(\slashoverback) = z\left(L(\smoothing)+L(\hsmoothing)\right)</math></center> |
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and by the initial condition <math>L(U)=1</math> where <math>U</math> is the unknot [[Image:BigCirc symbol.gif|20px]]. |
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and by the initial condition $L(\bigcirc)=1$. |
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<code>KnotTheory`</code> knows about the Kauffman polynomial: |
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{{Startup Note}} |
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\latexhtml{\small (for {\tt In[1]} see |
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Section~\ref{sec:Setup}.)}{\htmlref{{\tt In[1]}}{sec:Setup}} |
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%<* InOut[1] *> |
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\index{Kauffman, Louis} \index{Morrison, Scott} |
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{{HelpAndAbout| |
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n = 2 | |
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n1 = 3 | |
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in = <nowiki>Kauffman</nowiki> | |
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out= <nowiki>Kauffman[K][a, z] computes the Kauffman polynomial of a knot or link K, in the variables a and z.</nowiki> | |
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about= <nowiki>The Kauffman polynomial program was written by Scott Morrison.</nowiki>}} |
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Thus, for example, here's the Kauffman polynomial of the knot |
Thus, for example, here's the Kauffman polynomial of the knot [[5_2]]: |
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\hlink{../Knots/5.2.html}{$5_2$}: |
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{{InOut| |
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n = 4 | |
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in = <nowiki>Kauffman[Knot[5, 2]][a, z]</nowiki> | |
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out= <nowiki> 2 4 6 5 7 2 2 4 2 6 2 3 3 |
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-a + a + a - 2 a z - 2 a z + a z - a z - 2 a z + a z + |
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5 3 7 3 4 4 6 4 |
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2 a z + a z + a z + a z</nowiki>}} |
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{{Knot Image Pair|5_2|gif|T(8,3)|jpg}} |
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\vskip 6pt |
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\index{Jones polynomial} \index{Jones@{\tt Jones}} |
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polynomial via |
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$K$. Let us verify this fact for the torus knot |
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\hlink{../TorusKnots/8.3.html}{$T(8,3)$}: |
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{{In| |
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n = 5 | |
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in = <nowiki>K = TorusKnot[8, 3];</nowiki>}} |
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{{InOut| |
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n = 6 | |
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in = <nowiki>Simplify[{ |
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(-1)^(Length[Skeleton[K]]-1)Kauffman[K][-q^(-3/4), q^(1/4)+q^(-1/4)], |
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Jones[K][q] |
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}]</nowiki> | |
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out= <nowiki> 7 9 16 7 9 16 |
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{q + q - q , q + q - q }</nowiki>}} |
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{{note|Kauffman}} L. H. Kauffman, ''An invariant of regular isotopy'', Trans. Amer. Math. Soc. '''312''' (1990) 417-471. |
{{note|Kauffman}} L. H. Kauffman, ''An invariant of regular isotopy'', Trans. Amer. Math. Soc. '''312''' (1990) 417-471. |
Latest revision as of 17:23, 21 February 2013
The Kauffman polynomial (see [Kauffman]) of a knot or link is where is the writhe of (see How is the Jones Polynomial Computed?) and where is the regular isotopy invariant defined by the skein relations
(here is a strand and is the same strand with a kink added) and
and by the initial condition where is the unknot .
KnotTheory`
knows about the Kauffman polynomial:
(For In[1] see Setup)
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Thus, for example, here's the Kauffman polynomial of the knot 5_2:
In[4]:=
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Kauffman[Knot[5, 2]][a, z]
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Out[4]=
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2 4 6 5 7 2 2 4 2 6 2 3 3
-a + a + a - 2 a z - 2 a z + a z - a z - 2 a z + a z +
5 3 7 3 4 4 6 4
2 a z + a z + a z + a z
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5_2 |
T(8,3) |
It is well known that the Jones polynomial is related to the Kauffman polynomial via
where is some knot or link and where is the number of components of . Let us verify this fact for the torus knot T(8,3):
In[5]:=
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K = TorusKnot[8, 3];
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In[6]:=
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Simplify[{
(-1)^(Length[Skeleton[K]]-1)Kauffman[K][-q^(-3/4), q^(1/4)+q^(-1/4)],
Jones[K][q]
}]
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Out[6]=
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7 9 16 7 9 16
{q + q - q , q + q - q }
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[Kauffman] ^ L. H. Kauffman, An invariant of regular isotopy, Trans. Amer. Math. Soc. 312 (1990) 417-471.