K11a42
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Visit K11a42's page at Knotilus!
Visit K11a42's page at the original Knot Atlas! |
| K11a42 Quick Notes |
K11a42 Further Notes and Views
Knot presentations
| Planar diagram presentation | X4251 X8493 X14,6,15,5 X2837 X20,9,21,10 X16,11,17,12 X6,14,7,13 X12,15,13,16 X22,18,1,17 X10,19,11,20 X18,22,19,21 |
| Gauss code | 1, -4, 2, -1, 3, -7, 4, -2, 5, -10, 6, -8, 7, -3, 8, -6, 9, -11, 10, -5, 11, -9 |
| Dowker-Thistlethwaite code | 4 8 14 2 20 16 6 12 22 10 18 |
| Conway Notation | [22,21,2++] |
Three dimensional invariants
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Four dimensional invariants
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Polynomial invariants
| Alexander polynomial | [math]\displaystyle{ t^3-9 t^2+26 t-35+26 t^{-1} -9 t^{-2} + t^{-3} }[/math] |
| Conway polynomial | [math]\displaystyle{ z^6-3 z^4-z^2+1 }[/math] |
| 2nd Alexander ideal (db, data sources) | [math]\displaystyle{ \{1\} }[/math] |
| Determinant and Signature | { 107, 2 } |
| Jones polynomial | [math]\displaystyle{ -q^8+3 q^7-6 q^6+11 q^5-15 q^4+17 q^3-17 q^2+15 q-11+7 q^{-1} -3 q^{-2} + q^{-3} }[/math] |
| HOMFLY-PT polynomial (db, data sources) | [math]\displaystyle{ z^6 a^{-2} +2 z^4 a^{-2} -3 z^4 a^{-4} -2 z^4+a^2 z^2+3 z^2 a^{-2} -5 z^2 a^{-4} +3 z^2 a^{-6} -3 z^2+a^2+2 a^{-2} -3 a^{-4} +3 a^{-6} - a^{-8} -1 }[/math] |
| Kauffman polynomial (db, data sources) | [math]\displaystyle{ z^{10} a^{-2} +z^{10} a^{-4} +3 z^9 a^{-1} +6 z^9 a^{-3} +3 z^9 a^{-5} +7 z^8 a^{-2} +7 z^8 a^{-4} +4 z^8 a^{-6} +4 z^8+3 a z^7-5 z^7 a^{-3} +2 z^7 a^{-5} +4 z^7 a^{-7} +a^2 z^6-15 z^6 a^{-2} -10 z^6 a^{-4} +3 z^6 a^{-8} -7 z^6-8 a z^5-11 z^5 a^{-1} -5 z^5 a^{-3} -7 z^5 a^{-5} -4 z^5 a^{-7} +z^5 a^{-9} -3 a^2 z^4+4 z^4 a^{-2} -2 z^4 a^{-4} -10 z^4 a^{-6} -6 z^4 a^{-8} -z^4+6 a z^3+7 z^3 a^{-1} +5 z^3 a^{-3} +5 z^3 a^{-5} -z^3 a^{-7} -2 z^3 a^{-9} +3 a^2 z^2+3 z^2 a^{-2} +9 z^2 a^{-4} +11 z^2 a^{-6} +4 z^2 a^{-8} +4 z^2-a z-z a^{-1} -z a^{-3} -z a^{-5} +z a^{-7} +z a^{-9} -a^2-2 a^{-2} -3 a^{-4} -3 a^{-6} - a^{-8} -1 }[/math] |
| The A2 invariant | Data:K11a42/QuantumInvariant/A2/1,0 |
| The G2 invariant | Data:K11a42/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["K11a42"];
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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{ t^3-9 t^2+26 t-35+26 t^{-1} -9 t^{-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{ z^6-3 z^4-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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{ 107, 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^8+3 q^7-6 q^6+11 q^5-15 q^4+17 q^3-17 q^2+15 q-11+7 q^{-1} -3 q^{-2} + q^{-3} }[/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} +2 z^4 a^{-2} -3 z^4 a^{-4} -2 z^4+a^2 z^2+3 z^2 a^{-2} -5 z^2 a^{-4} +3 z^2 a^{-6} -3 z^2+a^2+2 a^{-2} -3 a^{-4} +3 a^{-6} - a^{-8} -1 }[/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} a^{-4} +3 z^9 a^{-1} +6 z^9 a^{-3} +3 z^9 a^{-5} +7 z^8 a^{-2} +7 z^8 a^{-4} +4 z^8 a^{-6} +4 z^8+3 a z^7-5 z^7 a^{-3} +2 z^7 a^{-5} +4 z^7 a^{-7} +a^2 z^6-15 z^6 a^{-2} -10 z^6 a^{-4} +3 z^6 a^{-8} -7 z^6-8 a z^5-11 z^5 a^{-1} -5 z^5 a^{-3} -7 z^5 a^{-5} -4 z^5 a^{-7} +z^5 a^{-9} -3 a^2 z^4+4 z^4 a^{-2} -2 z^4 a^{-4} -10 z^4 a^{-6} -6 z^4 a^{-8} -z^4+6 a z^3+7 z^3 a^{-1} +5 z^3 a^{-3} +5 z^3 a^{-5} -z^3 a^{-7} -2 z^3 a^{-9} +3 a^2 z^2+3 z^2 a^{-2} +9 z^2 a^{-4} +11 z^2 a^{-6} +4 z^2 a^{-8} +4 z^2-a z-z a^{-1} -z a^{-3} -z a^{-5} +z a^{-7} +z a^{-9} -a^2-2 a^{-2} -3 a^{-4} -3 a^{-6} - a^{-8} -1 }[/math] |
Vassiliev invariants
| V2 and V3: | (-1, 1) |
| 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 K11a42. 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, 42]] |
Out[2]= | 11 |
In[3]:= | PD[Knot[11, Alternating, 42]] |
Out[3]= | PD[X[4, 2, 5, 1], X[8, 4, 9, 3], X[14, 6, 15, 5], X[2, 8, 3, 7],X[20, 9, 21, 10], X[16, 11, 17, 12], X[6, 14, 7, 13], X[12, 15, 13, 16], X[22, 18, 1, 17], X[10, 19, 11, 20],X[18, 22, 19, 21]] |
In[4]:= | GaussCode[Knot[11, Alternating, 42]] |
Out[4]= | GaussCode[1, -4, 2, -1, 3, -7, 4, -2, 5, -10, 6, -8, 7, -3, 8, -6, 9, -11, 10, -5, 11, -9] |
In[5]:= | BR[Knot[11, Alternating, 42]] |
Out[5]= | BR[Knot[11, Alternating, 42]] |
In[6]:= | alex = Alexander[Knot[11, Alternating, 42]][t] |
Out[6]= | -3 9 26 2 3 |
In[7]:= | Conway[Knot[11, Alternating, 42]][z] |
Out[7]= | 2 4 6 1 - z - 3 z + z |
In[8]:= | Select[AllKnots[], (alex === Alexander[#][t])&] |
Out[8]= | {Knot[11, Alternating, 42]} |
In[9]:= | {KnotDet[Knot[11, Alternating, 42]], KnotSignature[Knot[11, Alternating, 42]]} |
Out[9]= | {107, 2} |
In[10]:= | J=Jones[Knot[11, Alternating, 42]][q] |
Out[10]= | -3 3 7 2 3 4 5 6 |
In[11]:= | Select[AllKnots[], (J === Jones[#][q] || (J /. q-> 1/q) === Jones[#][q])&] |
Out[11]= | {Knot[11, Alternating, 10], Knot[11, Alternating, 42]} |
In[12]:= | A2Invariant[Knot[11, Alternating, 42]][q] |
Out[12]= | -10 -6 3 2 2 4 6 8 14 16 |
In[13]:= | Kauffman[Knot[11, Alternating, 42]][a, z] |
Out[13]= | -8 3 3 2 2 z z z z z 2 |
In[14]:= | {Vassiliev[2][Knot[11, Alternating, 42]], Vassiliev[3][Knot[11, Alternating, 42]]} |
Out[14]= | {0, 1} |
In[15]:= | Kh[Knot[11, Alternating, 42]][q, t] |
Out[15]= | 3 1 2 1 5 2 6 5 q |


