K11a312
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a312's page at Knotilus! Visit K11a312's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X12,3,13,4 X16,5,17,6 X14,8,15,7 X18,9,19,10 X20,11,21,12 X2,13,3,14 X22,16,1,15 X4,17,5,18 X10,19,11,20 X8,21,9,22 |
| Gauss code | 1, -7, 2, -9, 3, -1, 4, -11, 5, -10, 6, -2, 7, -4, 8, -3, 9, -5, 10, -6, 11, -8 |
| Dowker-Thistlethwaite code | 6 12 16 14 18 20 2 22 4 10 8 |
| A Braid Representative | | ||||||
| A Morse Link Presentation |
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[edit] Three dimensional invariants
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[edit] Four dimensional invariants
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[edit] Polynomial invariants
| Alexander polynomial | 3t3−13t2 + 27t−33 + 27t−1−13t−2 + 3t−3 |
| Conway polynomial | 3z6 + 5z4 + 2z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 119, -2 } |
| Jones polynomial | −q2 + 3q−6 + 12q−1−16q−2 + 19q−3−19q−4 + 17q−5−13q−6 + 8q−7−4q−8 + q−9 |
| HOMFLY-PT polynomial (db, data sources) | z2a8 + a8−3z4a6−7z2a6−4a6 + 2z6a4 + 7z4a4 + 9z2a4 + 4a4 + z6a2 + 2z4a2 + z2a2−z4−2z2 |
| Kauffman polynomial (db, data sources) | z6a10−2z4a10 + z2a10 + 4z7a9−10z5a9 + 6z3a9 + 6z8a8−13z6a8 + 5z4a8−z2a8 + a8 + 5z9a7−6z7a7−5z5a7 + 2z3a7 + 2z10a6 + 7z8a6−27z6a6 + 29z4a6−18z2a6 + 4a6 + 11z9a5−28z7a5 + 31z5a5−16z3a5 + 2za5 + 2z10a4 + 8z8a4−33z6a4 + 48z4a4−25z2a4 + 4a4 + 6z9a3−13z7a3 + 16z5a3−6z3a3 + 2za3 + 7z8a2−17z6a2 + 20z4a2−7z2a2 + 5z7a−9z5a + 4z3a + 3z6−6z4 + 2z2 + z5a−1−2z3a−1 |
| The A2 invariant | Data:K11a312/QuantumInvariant/A2/1,0 |
| The G2 invariant | Data:K11a312/QuantumInvariant/G2/1,0 |
Further Quantum Invariants
Computer Talk
The above data is available with the Mathematica package
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]:=
| 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]:=
| K = Knot["K11a312"];
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In[4]:=
| Alexander[K][t]
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KnotTheory::loading: Loading precomputed data in PD4Knots`.
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Out[4]=
| 3t3−13t2 + 27t−33 + 27t−1−13t−2 + 3t−3 |
In[5]:=
| Conway[K][z]
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Out[5]=
| 3z6 + 5z4 + 2z2 + 1 |
In[6]:=
| 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]=
| {1} |
In[7]:=
| {KnotDet[K], KnotSignature[K]}
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Out[7]=
| { 119, -2 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| −q2 + 3q−6 + 12q−1−16q−2 + 19q−3−19q−4 + 17q−5−13q−6 + 8q−7−4q−8 + q−9 |
In[9]:=
| HOMFLYPT[K][a, z]
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KnotTheory::credits: The HOMFLYPT program was written by Scott Morrison.
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Out[9]=
| z2a8 + a8−3z4a6−7z2a6−4a6 + 2z6a4 + 7z4a4 + 9z2a4 + 4a4 + z6a2 + 2z4a2 + z2a2−z4−2z2 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| z6a10−2z4a10 + z2a10 + 4z7a9−10z5a9 + 6z3a9 + 6z8a8−13z6a8 + 5z4a8−z2a8 + a8 + 5z9a7−6z7a7−5z5a7 + 2z3a7 + 2z10a6 + 7z8a6−27z6a6 + 29z4a6−18z2a6 + 4a6 + 11z9a5−28z7a5 + 31z5a5−16z3a5 + 2za5 + 2z10a4 + 8z8a4−33z6a4 + 48z4a4−25z2a4 + 4a4 + 6z9a3−13z7a3 + 16z5a3−6z3a3 + 2za3 + 7z8a2−17z6a2 + 20z4a2−7z2a2 + 5z7a−9z5a + 4z3a + 3z6−6z4 + 2z2 + z5a−1−2z3a−1 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {}
Same Jones Polynomial (up to mirroring,
):
{}
Computer Talk
The above data is available with the Mathematica package
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]:=
| 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]:=
| K = Knot["K11a312"];
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In[4]:=
| {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]=
| { 3t3−13t2 + 27t−33 + 27t−1−13t−2 + 3t−3, −q2 + 3q−6 + 12q−1−16q−2 + 19q−3−19q−4 + 17q−5−13q−6 + 8q−7−4q−8 + q−9 } |
In[5]:=
| 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]=
| {} |
In[6]:=
| 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]=
| {} |
[edit] Khovanov Homology
| The coefficients of the monomials trqj are shown, along with their alternating sums χ (fixed j, alternation over r). The squares with yellow highlighting are those on the "critical diagonals", where j−2r = s + 1 or j−2r = s−1, where s = -2 is the signature of K11a312. 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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[edit] Computer Talk
Much of the above data can be recomputed by Mathematica using the packageKnotTheory`. See A Sample KnotTheory` Session.
[edit] 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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