K11a281
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![]() (Knotscape image) |
See the full Hoste-Thistlethwaite Table of 11 Crossing Knots. |
Knot presentations
| Planar diagram presentation | X6271 X10,3,11,4 X16,6,17,5 X12,8,13,7 X20,10,21,9 X2,11,3,12 X18,13,19,14 X4,16,5,15 X22,17,1,18 X8,20,9,19 X14,21,15,22 |
| Gauss code | 1, -6, 2, -8, 3, -1, 4, -10, 5, -2, 6, -4, 7, -11, 8, -3, 9, -7, 10, -5, 11, -9 |
| Dowker-Thistlethwaite code | 6 10 16 12 20 2 18 4 22 8 14 |
| A Braid Representative | |||||
| A Morse Link Presentation |
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Three dimensional invariants
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Four dimensional invariants
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Polynomial invariants
| Alexander polynomial | [math]\displaystyle{ -t^4+6 t^3-18 t^2+33 t-39+33 t^{-1} -18 t^{-2} +6 t^{-3} - t^{-4} }[/math] |
| Conway polynomial | [math]\displaystyle{ -z^8-2 z^6-2 z^4-z^2+1 }[/math] |
| 2nd Alexander ideal (db, data sources) | [math]\displaystyle{ \{1\} }[/math] |
| Determinant and Signature | { 155, 2 } |
| Jones polynomial | [math]\displaystyle{ q^7-4 q^6+10 q^5-17 q^4+22 q^3-25 q^2+25 q-21+16 q^{-1} -9 q^{-2} +4 q^{-3} - q^{-4} }[/math] |
| HOMFLY-PT polynomial (db, data sources) | [math]\displaystyle{ -z^8 a^{-2} -5 z^6 a^{-2} +z^6 a^{-4} +2 z^6-a^2 z^4-11 z^4 a^{-2} +3 z^4 a^{-4} +7 z^4-2 a^2 z^2-12 z^2 a^{-2} +4 z^2 a^{-4} +9 z^2-a^2-5 a^{-2} +2 a^{-4} +5 }[/math] |
| Kauffman polynomial (db, data sources) | [math]\displaystyle{ 3 z^{10} a^{-2} +3 z^{10}+6 a z^9+18 z^9 a^{-1} +12 z^9 a^{-3} +4 a^2 z^8+24 z^8 a^{-2} +19 z^8 a^{-4} +9 z^8+a^3 z^7-15 a z^7-41 z^7 a^{-1} -8 z^7 a^{-3} +17 z^7 a^{-5} -13 a^2 z^6-81 z^6 a^{-2} -33 z^6 a^{-4} +10 z^6 a^{-6} -51 z^6-3 a^3 z^5+6 a z^5+12 z^5 a^{-1} -25 z^5 a^{-3} -24 z^5 a^{-5} +4 z^5 a^{-7} +15 a^2 z^4+71 z^4 a^{-2} +19 z^4 a^{-4} -7 z^4 a^{-6} +z^4 a^{-8} +59 z^4+3 a^3 z^3+7 a z^3+12 z^3 a^{-1} +22 z^3 a^{-3} +14 z^3 a^{-5} -7 a^2 z^2-28 z^2 a^{-2} -7 z^2 a^{-4} +3 z^2 a^{-6} -25 z^2-a^3 z-3 a z-5 z a^{-1} -6 z a^{-3} -3 z a^{-5} +a^2+5 a^{-2} +2 a^{-4} +5 }[/math] |
| The A2 invariant | [math]\displaystyle{ -q^{12}+q^{10}-2 q^6+5 q^4-2 q^2+3+2 q^{-2} -4 q^{-4} +4 q^{-6} -6 q^{-8} +3 q^{-10} - q^{-12} -2 q^{-14} +4 q^{-16} -2 q^{-18} + q^{-20} }[/math] |
| The G2 invariant | Data:K11a281/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["K11a281"];
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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+6 t^3-18 t^2+33 t-39+33 t^{-1} -18 t^{-2} +6 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^8-2 z^6-2 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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{ 155, 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^7-4 q^6+10 q^5-17 q^4+22 q^3-25 q^2+25 q-21+16 q^{-1} -9 q^{-2} +4 q^{-3} - q^{-4} }[/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^8 a^{-2} -5 z^6 a^{-2} +z^6 a^{-4} +2 z^6-a^2 z^4-11 z^4 a^{-2} +3 z^4 a^{-4} +7 z^4-2 a^2 z^2-12 z^2 a^{-2} +4 z^2 a^{-4} +9 z^2-a^2-5 a^{-2} +2 a^{-4} +5 }[/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{ 3 z^{10} a^{-2} +3 z^{10}+6 a z^9+18 z^9 a^{-1} +12 z^9 a^{-3} +4 a^2 z^8+24 z^8 a^{-2} +19 z^8 a^{-4} +9 z^8+a^3 z^7-15 a z^7-41 z^7 a^{-1} -8 z^7 a^{-3} +17 z^7 a^{-5} -13 a^2 z^6-81 z^6 a^{-2} -33 z^6 a^{-4} +10 z^6 a^{-6} -51 z^6-3 a^3 z^5+6 a z^5+12 z^5 a^{-1} -25 z^5 a^{-3} -24 z^5 a^{-5} +4 z^5 a^{-7} +15 a^2 z^4+71 z^4 a^{-2} +19 z^4 a^{-4} -7 z^4 a^{-6} +z^4 a^{-8} +59 z^4+3 a^3 z^3+7 a z^3+12 z^3 a^{-1} +22 z^3 a^{-3} +14 z^3 a^{-5} -7 a^2 z^2-28 z^2 a^{-2} -7 z^2 a^{-4} +3 z^2 a^{-6} -25 z^2-a^3 z-3 a z-5 z a^{-1} -6 z a^{-3} -3 z a^{-5} +a^2+5 a^{-2} +2 a^{-4} +5 }[/math] |
"Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {K11a19, K11a25,}
Same Jones Polynomial (up to mirroring, [math]\displaystyle{ q\leftrightarrow q^{-1} }[/math]): {}
KnotTheory`. Your input (in red) is realistic; all else should have the same content as in a real mathematica session, but with different formatting.
(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 May 31, 2006, 14:15:20.091.
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In[3]:=
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K = Knot["K11a281"];
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In[4]:=
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{A = Alexander[K][t], J = Jones[K][q]}
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KnotTheory::loading: Loading precomputed data in PD4Knots`.
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[4]=
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{ [math]\displaystyle{ -t^4+6 t^3-18 t^2+33 t-39+33 t^{-1} -18 t^{-2} +6 t^{-3} - t^{-4} }[/math], [math]\displaystyle{ q^7-4 q^6+10 q^5-17 q^4+22 q^3-25 q^2+25 q-21+16 q^{-1} -9 q^{-2} +4 q^{-3} - q^{-4} }[/math] } |
In[5]:=
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DeleteCases[Select[AllKnots[], (A === Alexander[#][t]) &], K]
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KnotTheory::loading: Loading precomputed data in DTCode4KnotsTo11`.
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KnotTheory::credits: The GaussCode to PD conversion was written by Siddarth Sankaran at the University of Toronto in the summer of 2005.
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Out[5]=
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{K11a19, K11a25,} |
In[6]:=
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DeleteCases[
Select[
AllKnots[],
(J === Jones[#][q] || (J /. q -> 1/q) === Jones[#][q]) &
],
K
]
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KnotTheory::loading: Loading precomputed data in Jones4Knots11`.
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Out[6]=
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{} |
Vassiliev invariants
| V2 and V3: | (-1, -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]2 is the signature of K11a281. 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.
Modifying This Page
| Read me first: Modifying Knot Pages.
See/edit the Hoste-Thistlethwaite Knot Page master template (intermediate). See/edit the Hoste-Thistlethwaite_Splice_Base (expert). Back to the top. |
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