K11a316
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a316's page at Knotilus! Visit K11a316's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X12,4,13,3 X16,5,17,6 X20,8,21,7 X22,10,1,9 X4,12,5,11 X18,13,19,14 X10,15,11,16 X2,17,3,18 X14,19,15,20 X8,22,9,21 |
| Gauss code | 1, -9, 2, -6, 3, -1, 4, -11, 5, -8, 6, -2, 7, -10, 8, -3, 9, -7, 10, -4, 11, -5 |
| Dowker-Thistlethwaite code | 6 12 16 20 22 4 18 10 2 14 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 | t4−5t3 + 14t2−25t + 31−25t−1 + 14t−2−5t−3 + t−4 |
| Conway polynomial | z8 + 3z6 + 4z4 + 2z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 121, 0 } |
| Jones polynomial | q6−4q5 + 8q4−13q3 + 17q2−19q + 20−16q−1 + 12q−2−7q−3 + 3q−4−q−5 |
| HOMFLY-PT polynomial (db, data sources) | z8−a2z6−2z6a−2 + 6z6−4a2z4−8z4a−2 + z4a−4 + 15z4−6a2z2−11z2a−2 + 2z2a−4 + 17z2−3a2−5a−2 + a−4 + 8 |
| Kauffman polynomial (db, data sources) | 2z10a−2 + 2z10 + 6az9 + 11z9a−1 + 5z9a−3 + 8a2z8 + 7z8a−2 + 6z8a−4 + 9z8 + 6a3z7−10az7−26z7a−1−6z7a−3 + 4z7a−5 + 3a4z6−21a2z6−26z6a−2−13z6a−4 + z6a−6−36z6 + a5z5−13a3z5 + 4az5 + 23z5a−1−5z5a−3−10z5a−5−5a4z4 + 27a2z4 + 27z4a−2 + 5z4a−4−2z4a−6 + 52z4−2a5z3 + 10a3z3 + 10az3−5z3a−1 + 3z3a−3 + 6z3a−5−14a2z2−18z2a−2−z2a−4 + z2a−6−30z2−3a3z−5az−3za−1−za−3 + 3a2 + 5a−2 + a−4 + 8 |
| The A2 invariant | −q14 + q12−3q10 + q8 + q6−2q4 + 6q2−1 + 4q−2−2q−6 + 2q−8−4q−10 + q−12−q−16 + q−18 |
| The G2 invariant | Data:K11a316/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["K11a316"];
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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]=
| t4−5t3 + 14t2−25t + 31−25t−1 + 14t−2−5t−3 + t−4 |
In[5]:=
| Conway[K][z]
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Out[5]=
| z8 + 3z6 + 4z4 + 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]=
| { 121, 0 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| q6−4q5 + 8q4−13q3 + 17q2−19q + 20−16q−1 + 12q−2−7q−3 + 3q−4−q−5 |
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]=
| z8−a2z6−2z6a−2 + 6z6−4a2z4−8z4a−2 + z4a−4 + 15z4−6a2z2−11z2a−2 + 2z2a−4 + 17z2−3a2−5a−2 + a−4 + 8 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| 2z10a−2 + 2z10 + 6az9 + 11z9a−1 + 5z9a−3 + 8a2z8 + 7z8a−2 + 6z8a−4 + 9z8 + 6a3z7−10az7−26z7a−1−6z7a−3 + 4z7a−5 + 3a4z6−21a2z6−26z6a−2−13z6a−4 + z6a−6−36z6 + a5z5−13a3z5 + 4az5 + 23z5a−1−5z5a−3−10z5a−5−5a4z4 + 27a2z4 + 27z4a−2 + 5z4a−4−2z4a−6 + 52z4−2a5z3 + 10a3z3 + 10az3−5z3a−1 + 3z3a−3 + 6z3a−5−14a2z2−18z2a−2−z2a−4 + z2a−6−30z2−3a3z−5az−3za−1−za−3 + 3a2 + 5a−2 + a−4 + 8 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {K11a35,}
Same Jones Polynomial (up to mirroring,
):
{K11a35, K11a36,}
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["K11a316"];
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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]=
| { t4−5t3 + 14t2−25t + 31−25t−1 + 14t−2−5t−3 + t−4, q6−4q5 + 8q4−13q3 + 17q2−19q + 20−16q−1 + 12q−2−7q−3 + 3q−4−q−5 } |
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]=
| {K11a35,} |
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]=
| {K11a35, K11a36,} |
[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 = 0 is the signature of K11a316. 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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