L6a3
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Visit L6a3's page at Knotilus!
Visit L6a3's page at the original Knot Atlas! |
| The link L6a3 is [math]\displaystyle{ 6^2_1 }[/math] in the Rolfsen table of links. It is often seen in "Magen David" (star of David) necklaces. |
Ruberman, Cochran, Melvin, Akbulut, Gompf, Kirby [1] |
Rich Schwartz' "72" [2] |
Further images
Knot presentations
| Planar diagram presentation | X8192 X2,9,3,10 X10,3,11,4 X12,5,7,6 X6718 X4,11,5,12 |
| Gauss code | {1, -2, 3, -6, 4, -5}, {5, -1, 2, -3, 6, -4} |
Polynomial invariants
| Multivariable Alexander Polynomial (in [math]\displaystyle{ u }[/math], [math]\displaystyle{ v }[/math], [math]\displaystyle{ w }[/math], ...) | [math]\displaystyle{ \frac{-t(1)^2 t(2)^2-t(1) t(2)-1}{t(1) t(2)} }[/math] (db) |
| Jones polynomial | [math]\displaystyle{ -\frac{1}{q^{9/2}}-\frac{1}{q^{5/2}}-\frac{1}{q^{17/2}}+\frac{1}{q^{15/2}}-\frac{1}{q^{13/2}}+\frac{1}{q^{11/2}} }[/math] (db) |
| Signature | -5 (db) |
| HOMFLY-PT polynomial | [math]\displaystyle{ a^7 z^3+3 a^7 z+a^7 z^{-1} -a^5 z^5-5 a^5 z^3-6 a^5 z-a^5 z^{-1} }[/math] (db) |
| Kauffman polynomial | [math]\displaystyle{ -z a^{11}-z^2 a^{10}-z^3 a^9+z a^9-z^4 a^8+2 z^2 a^8-z^5 a^7+4 z^3 a^7-4 z a^7+a^7 z^{-1} -z^4 a^6+3 z^2 a^6-a^6-z^5 a^5+5 z^3 a^5-6 z a^5+a^5 z^{-1} }[/math] (db) |
Vassiliev invariants
| V2 and V3: | (0, [math]\displaystyle{ -\frac{177}{16} }[/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]-5 is the signature of L6a3. 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, 3]] |
Out[2]= | 6 |
In[3]:= | PD[Link[6, Alternating, 3]] |
Out[3]= | PD[X[8, 1, 9, 2], X[2, 9, 3, 10], X[10, 3, 11, 4], X[12, 5, 7, 6], X[6, 7, 1, 8], X[4, 11, 5, 12]] |
In[4]:= | GaussCode[Link[6, Alternating, 3]] |
Out[4]= | GaussCode[{1, -2, 3, -6, 4, -5}, {5, -1, 2, -3, 6, -4}] |
In[5]:= | BR[Link[6, Alternating, 3]] |
Out[5]= | BR[Link[6, Alternating, 3]] |
In[6]:= | alex = Alexander[Link[6, Alternating, 3]][t] |
Out[6]= | ComplexInfinity |
In[7]:= | Conway[Link[6, Alternating, 3]][z] |
Out[7]= | ComplexInfinity |
In[8]:= | Select[AllKnots[], (alex === Alexander[#][t])&] |
Out[8]= | {} |
In[9]:= | {KnotDet[Link[6, Alternating, 3]], KnotSignature[Link[6, Alternating, 3]]} |
Out[9]= | {Infinity, -5} |
In[10]:= | J=Jones[Link[6, Alternating, 3]][q] |
Out[10]= | -(17/2) -(15/2) -(13/2) -(11/2) -(9/2) -(5/2) -q + q - q + q - q - q |
In[11]:= | Select[AllKnots[], (J === Jones[#][q] || (J /. q-> 1/q) === Jones[#][q])&] |
Out[11]= | {} |
In[12]:= | A2Invariant[Link[6, Alternating, 3]][q] |
Out[12]= | -26 -24 -22 -16 -14 2 -10 -8 |
In[13]:= | Kauffman[Link[6, Alternating, 3]][a, z] |
Out[13]= | 5 76 a a 5 7 9 11 6 2 8 2 |
In[14]:= | {Vassiliev[2][Link[6, Alternating, 3]], Vassiliev[3][Link[6, Alternating, 3]]} |
Out[14]= | 177 |
In[15]:= | Kh[Link[6, Alternating, 3]][q, t] |
Out[15]= | -6 -4 1 1 1 1 1 1 |















