K11a90
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Visit K11a90's page at Knotilus!
Visit K11a90's page at the original Knot Atlas! |
| K11a90 Quick Notes |
K11a90 Further Notes and Views
Knot presentations
| Planar diagram presentation | X4251 X10,3,11,4 X12,6,13,5 X16,7,17,8 X18,9,19,10 X2,11,3,12 X22,14,1,13 X20,16,21,15 X8,17,9,18 X6,19,7,20 X14,22,15,21 |
| Gauss code | 1, -6, 2, -1, 3, -10, 4, -9, 5, -2, 6, -3, 7, -11, 8, -4, 9, -5, 10, -8, 11, -7 |
| Dowker-Thistlethwaite code | 4 10 12 16 18 2 22 20 8 6 14 |
| Conway Notation | [313112] |
Three dimensional invariants
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Four dimensional invariants
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Polynomial invariants
| Alexander polynomial | [math]\displaystyle{ 2 t^3-10 t^2+20 t-23+20 t^{-1} -10 t^{-2} +2 t^{-3} }[/math] |
| Conway polynomial | [math]\displaystyle{ 2 z^6+2 z^4-2 z^2+1 }[/math] |
| 2nd Alexander ideal (db, data sources) | [math]\displaystyle{ \{1\} }[/math] |
| Determinant and Signature | { 87, -2 } |
| Jones polynomial | [math]\displaystyle{ -q^4+3 q^3-5 q^2+9 q-11+13 q^{-1} -14 q^{-2} +12 q^{-3} -9 q^{-4} +6 q^{-5} -3 q^{-6} + q^{-7} }[/math] |
| HOMFLY-PT polynomial (db, data sources) | [math]\displaystyle{ z^2 a^6+a^6-2 z^4 a^4-4 z^2 a^4-a^4+z^6 a^2+2 z^4 a^2-a^2+z^6+3 z^4+3 z^2+2-z^4 a^{-2} -2 z^2 a^{-2} }[/math] |
| Kauffman polynomial (db, data sources) | [math]\displaystyle{ a^2 z^{10}+z^{10}+3 a^3 z^9+6 a z^9+3 z^9 a^{-1} +5 a^4 z^8+6 a^2 z^8+3 z^8 a^{-2} +4 z^8+6 a^5 z^7+a^3 z^7-16 a z^7-10 z^7 a^{-1} +z^7 a^{-3} +5 a^6 z^6-5 a^4 z^6-21 a^2 z^6-13 z^6 a^{-2} -24 z^6+3 a^7 z^5-9 a^5 z^5-14 a^3 z^5+10 a z^5+8 z^5 a^{-1} -4 z^5 a^{-3} +a^8 z^4-6 a^6 z^4-2 a^4 z^4+18 a^2 z^4+17 z^4 a^{-2} +30 z^4-3 a^7 z^3+8 a^5 z^3+14 a^3 z^3-3 a z^3-2 z^3 a^{-1} +4 z^3 a^{-3} -a^8 z^2+3 a^6 z^2+5 a^4 z^2-7 a^2 z^2-7 z^2 a^{-2} -15 z^2-3 a^5 z-3 a^3 z+a z+z a^{-1} -a^6-a^4+a^2+2 }[/math] |
| The A2 invariant | Data:K11a90/QuantumInvariant/A2/1,0 |
| The G2 invariant | Data:K11a90/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["K11a90"];
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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^3-10 t^2+20 t-23+20 t^{-1} -10 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+2 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{ \{1\} }[/math] |
In[7]:=
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{KnotDet[K], KnotSignature[K]}
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Out[7]=
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{ 87, -2 } |
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^4+3 q^3-5 q^2+9 q-11+13 q^{-1} -14 q^{-2} +12 q^{-3} -9 q^{-4} +6 q^{-5} -3 q^{-6} + q^{-7} }[/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^2 a^6+a^6-2 z^4 a^4-4 z^2 a^4-a^4+z^6 a^2+2 z^4 a^2-a^2+z^6+3 z^4+3 z^2+2-z^4 a^{-2} -2 z^2 a^{-2} }[/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{ a^2 z^{10}+z^{10}+3 a^3 z^9+6 a z^9+3 z^9 a^{-1} +5 a^4 z^8+6 a^2 z^8+3 z^8 a^{-2} +4 z^8+6 a^5 z^7+a^3 z^7-16 a z^7-10 z^7 a^{-1} +z^7 a^{-3} +5 a^6 z^6-5 a^4 z^6-21 a^2 z^6-13 z^6 a^{-2} -24 z^6+3 a^7 z^5-9 a^5 z^5-14 a^3 z^5+10 a z^5+8 z^5 a^{-1} -4 z^5 a^{-3} +a^8 z^4-6 a^6 z^4-2 a^4 z^4+18 a^2 z^4+17 z^4 a^{-2} +30 z^4-3 a^7 z^3+8 a^5 z^3+14 a^3 z^3-3 a z^3-2 z^3 a^{-1} +4 z^3 a^{-3} -a^8 z^2+3 a^6 z^2+5 a^4 z^2-7 a^2 z^2-7 z^2 a^{-2} -15 z^2-3 a^5 z-3 a^3 z+a z+z a^{-1} -a^6-a^4+a^2+2 }[/math] |
Vassiliev invariants
| V2 and V3: | (-2, 3) |
| 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 K11a90. 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, 90]] |
Out[2]= | 11 |
In[3]:= | PD[Knot[11, Alternating, 90]] |
Out[3]= | PD[X[4, 2, 5, 1], X[10, 3, 11, 4], X[12, 6, 13, 5], X[16, 7, 17, 8],X[18, 9, 19, 10], X[2, 11, 3, 12], X[22, 14, 1, 13], X[20, 16, 21, 15], X[8, 17, 9, 18], X[6, 19, 7, 20],X[14, 22, 15, 21]] |
In[4]:= | GaussCode[Knot[11, Alternating, 90]] |
Out[4]= | GaussCode[1, -6, 2, -1, 3, -10, 4, -9, 5, -2, 6, -3, 7, -11, 8, -4, 9, -5, 10, -8, 11, -7] |
In[5]:= | BR[Knot[11, Alternating, 90]] |
Out[5]= | BR[Knot[11, Alternating, 90]] |
In[6]:= | alex = Alexander[Knot[11, Alternating, 90]][t] |
Out[6]= | 2 10 20 2 3 |
In[7]:= | Conway[Knot[11, Alternating, 90]][z] |
Out[7]= | 2 4 6 1 - 2 z + 2 z + 2 z |
In[8]:= | Select[AllKnots[], (alex === Alexander[#][t])&] |
Out[8]= | {Knot[11, Alternating, 90], Knot[11, Alternating, 118]} |
In[9]:= | {KnotDet[Knot[11, Alternating, 90]], KnotSignature[Knot[11, Alternating, 90]]} |
Out[9]= | {87, -2} |
In[10]:= | J=Jones[Knot[11, Alternating, 90]][q] |
Out[10]= | -7 3 6 9 12 14 13 2 3 4 |
In[11]:= | Select[AllKnots[], (J === Jones[#][q] || (J /. q-> 1/q) === Jones[#][q])&] |
Out[11]= | {Knot[11, Alternating, 90]} |
In[12]:= | A2Invariant[Knot[11, Alternating, 90]][q] |
Out[12]= | -22 -18 2 -14 -10 3 -6 2 -2 2 4 |
In[13]:= | Kauffman[Knot[11, Alternating, 90]][a, z] |
Out[13]= | 22 4 6 z 3 5 2 7 z 2 2 |
In[14]:= | {Vassiliev[2][Knot[11, Alternating, 90]], Vassiliev[3][Knot[11, Alternating, 90]]} |
Out[14]= | {0, 3} |
In[15]:= | Kh[Knot[11, Alternating, 90]][q, t] |
Out[15]= | 6 8 1 2 1 4 2 5 4 |


