K11a263
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a263's page at Knotilus! Visit K11a263's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X8493 X16,6,17,5 X2837 X20,10,21,9 X22,12,1,11 X18,14,19,13 X4,16,5,15 X12,18,13,17 X14,20,15,19 X10,22,11,21 |
| Gauss code | 1, -4, 2, -8, 3, -1, 4, -2, 5, -11, 6, -9, 7, -10, 8, -3, 9, -7, 10, -5, 11, -6 |
| Dowker-Thistlethwaite code | 6 8 16 2 20 22 18 4 12 14 10 |
| 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 | 2t4−6t3 + 11t2−14t + 15−14t−1 + 11t−2−6t−3 + 2t−4 |
| Conway polynomial | 2z8 + 10z6 + 15z4 + 8z2 + 1 |
| 2nd Alexander ideal (db, data sources) | ![]() |
| Determinant and Signature | { 81, 8 } |
| Jones polynomial | −q15 + 3q14−6q13 + 10q12−12q11 + 12q10−13q9 + 10q8−7q7 + 5q6−q5 + q4 |
| HOMFLY-PT polynomial (db, data sources) | z8a−8 + z8a−10 + 7z6a−8 + 4z6a−10−z6a−12 + 18z4a−8−3z4a−12 + 20z2a−8−13z2a−10 + z2a−12 + 8a−8−11a−10 + 5a−12−a−14 |
| Kauffman polynomial (db, data sources) | z10a−10 + z10a−12 + z9a−9 + 5z9a−11 + 4z9a−13 + z8a−8−z8a−10 + 7z8a−12 + 9z8a−14−3z7a−9−14z7a−11 + z7a−13 + 12z7a−15−7z6a−8−11z6a−10−32z6a−12−18z6a−14 + 10z6a−16−3z5a−9−6z5a−11−36z5a−13−27z5a−15 + 6z5a−17 + 18z4a−8 + 28z4a−10 + 28z4a−12−15z4a−16 + 3z4a−18 + 16z3a−9 + 37z3a−11 + 43z3a−13 + 18z3a−15−3z3a−17 + z3a−19−20z2a−8−26z2a−10−7z2a−12 + 5z2a−14 + 6z2a−16−12za−9−22za−11−16za−13−6za−15 + 8a−8 + 11a−10 + 5a−12 + a−14 |
| The A2 invariant | q−14 + 4q−18 + q−20 + 4q−22 + q−24−2q−26−q−28−7q−30−2q−34 + 2q−36 + 3q−38 + q−42−2q−44 |
| The G2 invariant | Data:K11a263/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["K11a263"];
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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]=
| 2t4−6t3 + 11t2−14t + 15−14t−1 + 11t−2−6t−3 + 2t−4 |
In[5]:=
| Conway[K][z]
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Out[5]=
| 2z8 + 10z6 + 15z4 + 8z2 + 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]=
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In[7]:=
| {KnotDet[K], KnotSignature[K]}
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Out[7]=
| { 81, 8 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| −q15 + 3q14−6q13 + 10q12−12q11 + 12q10−13q9 + 10q8−7q7 + 5q6−q5 + q4 |
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]=
| z8a−8 + z8a−10 + 7z6a−8 + 4z6a−10−z6a−12 + 18z4a−8−3z4a−12 + 20z2a−8−13z2a−10 + z2a−12 + 8a−8−11a−10 + 5a−12−a−14 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| z10a−10 + z10a−12 + z9a−9 + 5z9a−11 + 4z9a−13 + z8a−8−z8a−10 + 7z8a−12 + 9z8a−14−3z7a−9−14z7a−11 + z7a−13 + 12z7a−15−7z6a−8−11z6a−10−32z6a−12−18z6a−14 + 10z6a−16−3z5a−9−6z5a−11−36z5a−13−27z5a−15 + 6z5a−17 + 18z4a−8 + 28z4a−10 + 28z4a−12−15z4a−16 + 3z4a−18 + 16z3a−9 + 37z3a−11 + 43z3a−13 + 18z3a−15−3z3a−17 + z3a−19−20z2a−8−26z2a−10−7z2a−12 + 5z2a−14 + 6z2a−16−12za−9−22za−11−16za−13−6za−15 + 8a−8 + 11a−10 + 5a−12 + a−14 |
[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["K11a263"];
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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]=
| { 2t4−6t3 + 11t2−14t + 15−14t−1 + 11t−2−6t−3 + 2t−4, −q15 + 3q14−6q13 + 10q12−12q11 + 12q10−13q9 + 10q8−7q7 + 5q6−q5 + q4 } |
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 = 8 is the signature of K11a263. 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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