L6a5
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Visit L6a5's page at Knotilus!
Visit L6a5's page at the original Knot Atlas! |
| L6a5 is [math]\displaystyle{ 6^3_1 }[/math] in the Rolfsen table of links. It is a closed three-link chain. |
Knot presentations
| Planar diagram presentation | X6172 X10,3,11,4 X12,7,9,8 X8,11,5,12 X2536 X4,9,1,10 |
| Gauss code | {1, -5, 2, -6}, {5, -1, 3, -4}, {6, -2, 4, -3} |
Polynomial invariants
| Multivariable Alexander Polynomial (in [math]\displaystyle{ u }[/math], [math]\displaystyle{ v }[/math], [math]\displaystyle{ w }[/math], ...) | [math]\displaystyle{ \frac{t(2) t(1)+t(3) t(1)-t(1)-t(2)+t(2) t(3)-t(3)}{\sqrt{t(1)} \sqrt{t(2)} \sqrt{t(3)}} }[/math] (db) |
| Jones polynomial | [math]\displaystyle{ q^{-1} -2 q^{-2} +3 q^{-3} - q^{-4} +3 q^{-5} - q^{-6} + q^{-7} }[/math] (db) |
| Signature | -2 (db) |
| HOMFLY-PT polynomial | [math]\displaystyle{ a^8 z^{-2} -2 a^6 z^{-2} -3 a^6+2 a^4 z^2+a^4 z^{-2} +3 a^4+a^2 z^2 }[/math] (db) |
| Kauffman polynomial | [math]\displaystyle{ z^4 a^8-3 z^2 a^8-a^8 z^{-2} +3 a^8+z^5 a^7-z^3 a^7-3 z a^7+2 a^7 z^{-1} +4 z^4 a^6-9 z^2 a^6-2 a^6 z^{-2} +5 a^6+z^5 a^5+z^3 a^5-3 z a^5+2 a^5 z^{-1} +3 z^4 a^4-5 z^2 a^4-a^4 z^{-2} +3 a^4+2 z^3 a^3+z^2 a^2 }[/math] (db) |
Vassiliev invariants
| V2 and V3: | (0, [math]\displaystyle{ \frac{27}{2} }[/math]) |
| V2,1 through V6,9: |
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V2,1 through V6,9 were provided by Petr Dunin-Barkowski <barkovs@itep.ru>, Andrey Smirnov <asmirnov@itep.ru>, and Alexei Sleptsov <sleptsov@itep.ru> and uploaded on October 2010 by User:Drorbn. Note that they are normalized differently than V2 and V3.
Khovanov Homology
| The coefficients of the monomials [math]\displaystyle{ t^rq^j }[/math] are shown, along with their alternating sums [math]\displaystyle{ \chi }[/math] (fixed [math]\displaystyle{ j }[/math], alternation over [math]\displaystyle{ r }[/math]). The squares with yellow highlighting are those on the "critical diagonals", where [math]\displaystyle{ j-2r=s+1 }[/math] or [math]\displaystyle{ j-2r=s-1 }[/math], where [math]\displaystyle{ s= }[/math]-2 is the signature of L6a5. Nonzero entries off the critical diagonals (if any exist) are highlighted in red. |
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| Integral Khovanov Homology
(db, data source) |
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Computer Talk
Much of the above data can be recomputed by Mathematica using the package KnotTheory`. See A Sample KnotTheory` Session.
[math]\displaystyle{ \textrm{Include}(\textrm{ColouredJonesM.mhtml}) }[/math]
In[1]:= |
<< KnotTheory` |
Loading KnotTheory` (version of August 17, 2005, 14:44:34)... | |
In[2]:= | Crossings[Link[6, Alternating, 5]] |
Out[2]= | 6 |
In[3]:= | PD[Link[6, Alternating, 5]] |
Out[3]= | PD[X[6, 1, 7, 2], X[10, 3, 11, 4], X[12, 7, 9, 8], X[8, 11, 5, 12], X[2, 5, 3, 6], X[4, 9, 1, 10]] |
In[4]:= | GaussCode[Link[6, Alternating, 5]] |
Out[4]= | GaussCode[{1, -5, 2, -6}, {5, -1, 3, -4}, {6, -2, 4, -3}] |
In[5]:= | BR[Link[6, Alternating, 5]] |
Out[5]= | BR[Link[6, Alternating, 5]] |
In[6]:= | alex = Alexander[Link[6, Alternating, 5]][t] |
Out[6]= | ComplexInfinity |
In[7]:= | Conway[Link[6, Alternating, 5]][z] |
Out[7]= | ComplexInfinity |
In[8]:= | Select[AllKnots[], (alex === Alexander[#][t])&] |
Out[8]= | {} |
In[9]:= | {KnotDet[Link[6, Alternating, 5]], KnotSignature[Link[6, Alternating, 5]]} |
Out[9]= | {Infinity, -2} |
In[10]:= | J=Jones[Link[6, Alternating, 5]][q] |
Out[10]= | -7 -6 3 -4 3 2 1 |
In[11]:= | Select[AllKnots[], (J === Jones[#][q] || (J /. q-> 1/q) === Jones[#][q])&] |
Out[11]= | {} |
In[12]:= | A2Invariant[Link[6, Alternating, 5]][q] |
Out[12]= | -24 3 3 4 5 4 4 2 -8 -4 -2 |
In[13]:= | Kauffman[Link[6, Alternating, 5]][a, z] |
Out[13]= | 4 6 8 5 74 6 8 a 2 a a 2 a 2 a 5 7 |
In[14]:= | {Vassiliev[2][Link[6, Alternating, 5]], Vassiliev[3][Link[6, Alternating, 5]]} |
Out[14]= | 27 |
In[15]:= | Kh[Link[6, Alternating, 5]][q, t] |
Out[15]= | -3 1 1 1 3 3 1 2 1 |






