K11a62
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Visit K11a62's page at Knotilus!
Visit K11a62's page at the original Knot Atlas! |
| K11a62 Quick Notes |
K11a62 Further Notes and Views
Knot presentations
| Planar diagram presentation | X4251 X8394 X16,5,17,6 X10,8,11,7 X2,9,3,10 X18,11,19,12 X20,13,21,14 X22,15,1,16 X6,17,7,18 X12,19,13,20 X14,21,15,22 |
| Gauss code | 1, -5, 2, -1, 3, -9, 4, -2, 5, -4, 6, -10, 7, -11, 8, -3, 9, -6, 10, -7, 11, -8 |
| Dowker-Thistlethwaite code | 4 8 16 10 2 18 20 22 6 12 14 |
| Conway Notation | [5,22,2] |
Three dimensional invariants
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Four dimensional invariants
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Polynomial invariants
| Alexander polynomial | [math]\displaystyle{ -t^4+5 t^3-8 t^2+9 t-9+9 t^{-1} -8 t^{-2} +5 t^{-3} - t^{-4} }[/math] |
| Conway polynomial | [math]\displaystyle{ -z^8-3 z^6+2 z^4+6 z^2+1 }[/math] |
| 2nd Alexander ideal (db, data sources) | [math]\displaystyle{ \{1\} }[/math] |
| Determinant and Signature | { 55, -6 } |
| Jones polynomial | [math]\displaystyle{ q^{-1} -2 q^{-2} +4 q^{-3} -5 q^{-4} +7 q^{-5} -8 q^{-6} +8 q^{-7} -7 q^{-8} +6 q^{-9} -4 q^{-10} +2 q^{-11} - q^{-12} }[/math] |
| HOMFLY-PT polynomial (db, data sources) | [math]\displaystyle{ -z^4 a^{10}-4 z^2 a^{10}-3 a^{10}+2 z^6 a^8+10 z^4 a^8+14 z^2 a^8+6 a^8-z^8 a^6-6 z^6 a^6-12 z^4 a^6-11 z^2 a^6-5 a^6+z^6 a^4+5 z^4 a^4+7 z^2 a^4+3 a^4 }[/math] |
| Kauffman polynomial (db, data sources) | [math]\displaystyle{ z^3 a^{15}-z a^{15}+2 z^4 a^{14}-z^2 a^{14}+3 z^5 a^{13}-2 z^3 a^{13}+z a^{13}+4 z^6 a^{12}-6 z^4 a^{12}+4 z^2 a^{12}+4 z^7 a^{11}-7 z^5 a^{11}+2 z^3 a^{11}+4 z^8 a^{10}-11 z^6 a^{10}+10 z^4 a^{10}-9 z^2 a^{10}+3 a^{10}+3 z^9 a^9-9 z^7 a^9+6 z^5 a^9-3 z^3 a^9+z^{10} a^8+2 z^8 a^8-24 z^6 a^8+41 z^4 a^8-27 z^2 a^8+6 a^8+5 z^9 a^7-24 z^7 a^7+34 z^5 a^7-17 z^3 a^7+3 z a^7+z^{10} a^6-z^8 a^6-15 z^6 a^6+35 z^4 a^6-23 z^2 a^6+5 a^6+2 z^9 a^5-11 z^7 a^5+18 z^5 a^5-9 z^3 a^5+z a^5+z^8 a^4-6 z^6 a^4+12 z^4 a^4-10 z^2 a^4+3 a^4 }[/math] |
| The A2 invariant | [math]\displaystyle{ -q^{36}-q^{34}-q^{30}+q^{28}+2 q^{24}+q^{22}-q^{20}+q^{18}-2 q^{16}+q^{14}+q^{10}+q^8+q^4 }[/math] |
| The G2 invariant | [math]\displaystyle{ q^{196}-q^{194}+2 q^{192}-2 q^{190}+q^{188}-2 q^{184}+4 q^{182}-5 q^{180}+6 q^{178}-6 q^{176}+3 q^{174}+2 q^{172}-6 q^{170}+11 q^{168}-12 q^{166}+10 q^{164}-8 q^{162}-q^{160}+7 q^{158}-14 q^{156}+15 q^{154}-12 q^{152}+5 q^{150}-6 q^{146}+8 q^{144}-8 q^{142}+6 q^{140}-6 q^{138}+4 q^{136}-5 q^{134}+3 q^{132}+2 q^{130}-8 q^{128}+14 q^{126}-13 q^{124}+7 q^{122}+q^{120}-10 q^{118}+11 q^{116}-4 q^{114}-5 q^{112}+14 q^{110}-14 q^{108}+7 q^{106}+11 q^{104}-24 q^{102}+31 q^{100}-26 q^{98}+12 q^{96}+7 q^{94}-21 q^{92}+33 q^{90}-30 q^{88}+23 q^{86}-9 q^{84}-7 q^{82}+19 q^{80}-24 q^{78}+18 q^{76}-9 q^{74}-6 q^{72}+16 q^{70}-18 q^{68}+7 q^{66}+10 q^{64}-25 q^{62}+29 q^{60}-22 q^{58}+q^{56}+20 q^{54}-34 q^{52}+38 q^{50}-26 q^{48}+9 q^{46}+11 q^{44}-22 q^{42}+25 q^{40}-17 q^{38}+10 q^{36}-4 q^{32}+6 q^{30}-5 q^{28}+4 q^{26}-q^{24}+q^{22} }[/math] |
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["K11a62"];
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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^4+5 t^3-8 t^2+9 t-9+9 t^{-1} -8 t^{-2} +5 t^{-3} - t^{-4} }[/math] |
In[5]:=
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Conway[K][z]
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Out[5]=
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[math]\displaystyle{ -z^8-3 z^6+2 z^4+6 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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{ 55, -6 } |
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^{-1} -2 q^{-2} +4 q^{-3} -5 q^{-4} +7 q^{-5} -8 q^{-6} +8 q^{-7} -7 q^{-8} +6 q^{-9} -4 q^{-10} +2 q^{-11} - q^{-12} }[/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^4 a^{10}-4 z^2 a^{10}-3 a^{10}+2 z^6 a^8+10 z^4 a^8+14 z^2 a^8+6 a^8-z^8 a^6-6 z^6 a^6-12 z^4 a^6-11 z^2 a^6-5 a^6+z^6 a^4+5 z^4 a^4+7 z^2 a^4+3 a^4 }[/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^3 a^{15}-z a^{15}+2 z^4 a^{14}-z^2 a^{14}+3 z^5 a^{13}-2 z^3 a^{13}+z a^{13}+4 z^6 a^{12}-6 z^4 a^{12}+4 z^2 a^{12}+4 z^7 a^{11}-7 z^5 a^{11}+2 z^3 a^{11}+4 z^8 a^{10}-11 z^6 a^{10}+10 z^4 a^{10}-9 z^2 a^{10}+3 a^{10}+3 z^9 a^9-9 z^7 a^9+6 z^5 a^9-3 z^3 a^9+z^{10} a^8+2 z^8 a^8-24 z^6 a^8+41 z^4 a^8-27 z^2 a^8+6 a^8+5 z^9 a^7-24 z^7 a^7+34 z^5 a^7-17 z^3 a^7+3 z a^7+z^{10} a^6-z^8 a^6-15 z^6 a^6+35 z^4 a^6-23 z^2 a^6+5 a^6+2 z^9 a^5-11 z^7 a^5+18 z^5 a^5-9 z^3 a^5+z a^5+z^8 a^4-6 z^6 a^4+12 z^4 a^4-10 z^2 a^4+3 a^4 }[/math] |
Vassiliev invariants
| V2 and V3: | (6, -17) |
| 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]-6 is the signature of K11a62. 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[Knot[11, Alternating, 62]] |
Out[2]= | 11 |
In[3]:= | PD[Knot[11, Alternating, 62]] |
Out[3]= | PD[X[4, 2, 5, 1], X[8, 3, 9, 4], X[16, 5, 17, 6], X[10, 8, 11, 7],X[2, 9, 3, 10], X[18, 11, 19, 12], X[20, 13, 21, 14], X[22, 15, 1, 16], X[6, 17, 7, 18], X[12, 19, 13, 20],X[14, 21, 15, 22]] |
In[4]:= | GaussCode[Knot[11, Alternating, 62]] |
Out[4]= | GaussCode[1, -5, 2, -1, 3, -9, 4, -2, 5, -4, 6, -10, 7, -11, 8, -3, 9, -6, 10, -7, 11, -8] |
In[5]:= | BR[Knot[11, Alternating, 62]] |
Out[5]= | BR[Knot[11, Alternating, 62]] |
In[6]:= | alex = Alexander[Knot[11, Alternating, 62]][t] |
Out[6]= | -4 5 8 9 2 3 4 |
In[7]:= | Conway[Knot[11, Alternating, 62]][z] |
Out[7]= | 2 4 6 8 1 + 6 z + 2 z - 3 z - z |
In[8]:= | Select[AllKnots[], (alex === Alexander[#][t])&] |
Out[8]= | {Knot[11, Alternating, 62]} |
In[9]:= | {KnotDet[Knot[11, Alternating, 62]], KnotSignature[Knot[11, Alternating, 62]]} |
Out[9]= | {55, -6} |
In[10]:= | J=Jones[Knot[11, Alternating, 62]][q] |
Out[10]= | -12 2 4 6 7 8 8 7 5 4 2 1 |
In[11]:= | Select[AllKnots[], (J === Jones[#][q] || (J /. q-> 1/q) === Jones[#][q])&] |
Out[11]= | {Knot[11, Alternating, 62]} |
In[12]:= | A2Invariant[Knot[11, Alternating, 62]][q] |
Out[12]= | -36 -34 -30 -28 2 -22 -20 -18 2 -14 |
In[13]:= | Kauffman[Knot[11, Alternating, 62]][a, z] |
Out[13]= | 4 6 8 10 5 7 13 15 4 2 |
In[14]:= | {Vassiliev[2][Knot[11, Alternating, 62]], Vassiliev[3][Knot[11, Alternating, 62]]} |
Out[14]= | {0, -17} |
In[15]:= | Kh[Knot[11, Alternating, 62]][q, t] |
Out[15]= | 2 3 1 1 1 3 1 3 |


