K11a87
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Visit K11a87's page at Knotilus!
Visit K11a87's page at the original Knot Atlas! |
| K11a87 Quick Notes |
K11a87 Further Notes and Views
Knot presentations
| Planar diagram presentation | X4251 X10,3,11,4 X12,6,13,5 X16,8,17,7 X18,10,19,9 X2,11,3,12 X20,13,21,14 X8,16,9,15 X6,18,7,17 X22,19,1,20 X14,21,15,22 |
| Gauss code | 1, -6, 2, -1, 3, -9, 4, -8, 5, -2, 6, -3, 7, -11, 8, -4, 9, -5, 10, -7, 11, -10 |
| Dowker-Thistlethwaite code | 4 10 12 16 18 2 20 8 6 22 14 |
| Conway Notation | [31,211,21] |
Three dimensional invariants
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Four dimensional invariants
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Polynomial invariants
| Alexander polynomial | [math]\displaystyle{ -2 t^3+11 t^2-28 t+39-28 t^{-1} +11 t^{-2} -2 t^{-3} }[/math] |
| Conway polynomial | [math]\displaystyle{ -2 z^6-z^4-2 z^2+1 }[/math] |
| 2nd Alexander ideal (db, data sources) | [math]\displaystyle{ \left\{2,t^2+t+1\right\} }[/math] |
| Determinant and Signature | { 121, 0 } |
| Jones polynomial | [math]\displaystyle{ q^6-3 q^5+7 q^4-12 q^3+16 q^2-19 q+20-17 q^{-1} +13 q^{-2} -8 q^{-3} +4 q^{-4} - q^{-5} }[/math] |
| HOMFLY-PT polynomial (db, data sources) | [math]\displaystyle{ -z^6 a^{-2} -z^6+2 a^2 z^4-3 z^4 a^{-2} +z^4 a^{-4} -z^4-a^4 z^2+2 a^2 z^2-6 z^2 a^{-2} +2 z^2 a^{-4} +z^2-4 a^{-2} +2 a^{-4} +3 }[/math] |
| Kauffman polynomial (db, data sources) | [math]\displaystyle{ z^{10} a^{-2} +z^{10}+4 a z^9+8 z^9 a^{-1} +4 z^9 a^{-3} +7 a^2 z^8+12 z^8 a^{-2} +5 z^8 a^{-4} +14 z^8+7 a^3 z^7+6 a z^7-8 z^7 a^{-1} -4 z^7 a^{-3} +3 z^7 a^{-5} +4 a^4 z^6-7 a^2 z^6-37 z^6 a^{-2} -13 z^6 a^{-4} +z^6 a^{-6} -34 z^6+a^5 z^5-11 a^3 z^5-22 a z^5-8 z^5 a^{-1} -6 z^5 a^{-3} -8 z^5 a^{-5} -6 a^4 z^4-a^2 z^4+41 z^4 a^{-2} +12 z^4 a^{-4} -3 z^4 a^{-6} +31 z^4-a^5 z^3+5 a^3 z^3+16 a z^3+12 z^3 a^{-1} +8 z^3 a^{-3} +6 z^3 a^{-5} +2 a^4 z^2+a^2 z^2-21 z^2 a^{-2} -7 z^2 a^{-4} +2 z^2 a^{-6} -13 z^2-a^3 z-3 a z-3 z a^{-1} -3 z a^{-3} -2 z a^{-5} +4 a^{-2} +2 a^{-4} +3 }[/math] |
| The A2 invariant | Data:K11a87/QuantumInvariant/A2/1,0 |
| The G2 invariant | Data:K11a87/QuantumInvariant/G2/1,0 |
KnotTheory`, as shown in the (simulated) Mathematica session below. Your input (in red) is realistic; all else should have the same content as in a real mathematica session, but with different formatting. This Mathematica session is also available (albeit only for the knot 5_2) as the notebook PolynomialInvariantsSession.nb.
(The path below may be different on your system, and possibly also the KnotTheory` date)
In[1]:=
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AppendTo[$Path, "C:/drorbn/projects/KAtlas/"];
<< KnotTheory`
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Loading KnotTheory` version of August 31, 2006, 11:25:27.5625.
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In[3]:=
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K = Knot["K11a87"];
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In[4]:=
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Alexander[K][t]
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KnotTheory::loading: Loading precomputed data in PD4Knots`.
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Out[4]=
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[math]\displaystyle{ -2 t^3+11 t^2-28 t+39-28 t^{-1} +11 t^{-2} -2 t^{-3} }[/math] |
In[5]:=
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Conway[K][z]
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Out[5]=
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[math]\displaystyle{ -2 z^6-z^4-2 z^2+1 }[/math] |
In[6]:=
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Alexander[K, 2][t]
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KnotTheory::credits: The program Alexander[K, r] to compute Alexander ideals was written by Jana Archibald at the University of Toronto in the summer of 2005.
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Out[6]=
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[math]\displaystyle{ \left\{2,t^2+t+1\right\} }[/math] |
In[7]:=
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{KnotDet[K], KnotSignature[K]}
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Out[7]=
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{ 121, 0 } |
In[8]:=
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Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
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[math]\displaystyle{ q^6-3 q^5+7 q^4-12 q^3+16 q^2-19 q+20-17 q^{-1} +13 q^{-2} -8 q^{-3} +4 q^{-4} - q^{-5} }[/math] |
In[9]:=
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HOMFLYPT[K][a, z]
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KnotTheory::credits: The HOMFLYPT program was written by Scott Morrison.
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Out[9]=
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[math]\displaystyle{ -z^6 a^{-2} -z^6+2 a^2 z^4-3 z^4 a^{-2} +z^4 a^{-4} -z^4-a^4 z^2+2 a^2 z^2-6 z^2 a^{-2} +2 z^2 a^{-4} +z^2-4 a^{-2} +2 a^{-4} +3 }[/math] |
In[10]:=
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Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
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[math]\displaystyle{ z^{10} a^{-2} +z^{10}+4 a z^9+8 z^9 a^{-1} +4 z^9 a^{-3} +7 a^2 z^8+12 z^8 a^{-2} +5 z^8 a^{-4} +14 z^8+7 a^3 z^7+6 a z^7-8 z^7 a^{-1} -4 z^7 a^{-3} +3 z^7 a^{-5} +4 a^4 z^6-7 a^2 z^6-37 z^6 a^{-2} -13 z^6 a^{-4} +z^6 a^{-6} -34 z^6+a^5 z^5-11 a^3 z^5-22 a z^5-8 z^5 a^{-1} -6 z^5 a^{-3} -8 z^5 a^{-5} -6 a^4 z^4-a^2 z^4+41 z^4 a^{-2} +12 z^4 a^{-4} -3 z^4 a^{-6} +31 z^4-a^5 z^3+5 a^3 z^3+16 a z^3+12 z^3 a^{-1} +8 z^3 a^{-3} +6 z^3 a^{-5} +2 a^4 z^2+a^2 z^2-21 z^2 a^{-2} -7 z^2 a^{-4} +2 z^2 a^{-6} -13 z^2-a^3 z-3 a z-3 z a^{-1} -3 z a^{-3} -2 z a^{-5} +4 a^{-2} +2 a^{-4} +3 }[/math] |
Vassiliev invariants
| V2 and V3: | (-2, -2) |
| 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]0 is the signature of K11a87. Nonzero entries off the critical diagonals (if any exist) are highlighted in red. |
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| Integral Khovanov Homology
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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[Knot[11, Alternating, 87]] |
Out[2]= | 11 |
In[3]:= | PD[Knot[11, Alternating, 87]] |
Out[3]= | PD[X[4, 2, 5, 1], X[10, 3, 11, 4], X[12, 6, 13, 5], X[16, 8, 17, 7],X[18, 10, 19, 9], X[2, 11, 3, 12], X[20, 13, 21, 14],X[8, 16, 9, 15], X[6, 18, 7, 17], X[22, 19, 1, 20], X[14, 21, 15, 22]] |
In[4]:= | GaussCode[Knot[11, Alternating, 87]] |
Out[4]= | GaussCode[1, -6, 2, -1, 3, -9, 4, -8, 5, -2, 6, -3, 7, -11, 8, -4, 9, -5, 10, -7, 11, -10] |
In[5]:= | BR[Knot[11, Alternating, 87]] |
Out[5]= | BR[Knot[11, Alternating, 87]] |
In[6]:= | alex = Alexander[Knot[11, Alternating, 87]][t] |
Out[6]= | 2 11 28 2 3 |
In[7]:= | Conway[Knot[11, Alternating, 87]][z] |
Out[7]= | 2 4 6 1 - 2 z - z - 2 z |
In[8]:= | Select[AllKnots[], (alex === Alexander[#][t])&] |
Out[8]= | {Knot[11, Alternating, 87]} |
In[9]:= | {KnotDet[Knot[11, Alternating, 87]], KnotSignature[Knot[11, Alternating, 87]]} |
Out[9]= | {121, 0} |
In[10]:= | J=Jones[Knot[11, Alternating, 87]][q] |
Out[10]= | -5 4 8 13 17 2 3 4 5 6 |
In[11]:= | Select[AllKnots[], (J === Jones[#][q] || (J /. q-> 1/q) === Jones[#][q])&] |
Out[11]= | {Knot[11, Alternating, 28], Knot[11, Alternating, 87],
Knot[11, Alternating, 96]} |
In[12]:= | A2Invariant[Knot[11, Alternating, 87]][q] |
Out[12]= | -16 -14 2 3 2 2 5 2 4 6 |
In[13]:= | Kauffman[Knot[11, Alternating, 87]][a, z] |
Out[13]= | 2 22 4 2 z 3 z 3 z 3 2 2 z 7 z |
In[14]:= | {Vassiliev[2][Knot[11, Alternating, 87]], Vassiliev[3][Knot[11, Alternating, 87]]} |
Out[14]= | {0, -2} |
In[15]:= | Kh[Knot[11, Alternating, 87]][q, t] |
Out[15]= | 11 1 3 1 5 3 8 5 |


