K11a331
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a331's page at Knotilus! Visit K11a331's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X12,4,13,3 X18,5,19,6 X22,8,1,7 X16,9,17,10 X4,12,5,11 X20,13,21,14 X10,15,11,16 X8,17,9,18 X2,19,3,20 X14,21,15,22 |
| Gauss code | 1, -10, 2, -6, 3, -1, 4, -9, 5, -8, 6, -2, 7, -11, 8, -5, 9, -3, 10, -7, 11, -4 |
| Dowker-Thistlethwaite code | 6 12 18 22 16 4 20 10 8 2 14 |
| 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 | 2t3−11t2 + 27t−35 + 27t−1−11t−2 + 2t−3 |
| Conway polynomial | 2z6 + z4 + z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 115, -2 } |
| Jones polynomial | q3−3q2 + 7q−12 + 16q−1−18q−2 + 19q−3−16q−4 + 12q−5−7q−6 + 3q−7−q−8 |
| HOMFLY-PT polynomial (db, data sources) | −z4a6−2z2a6−2a6 + z6a4 + 3z4a4 + 6z2a4 + 4a4 + z6a2 + z4a2−z2a2−a2−2z4−3z2−1 + z2a−2 + a−2 |
| Kauffman polynomial (db, data sources) | 2a4z10 + 2a2z10 + 6a5z9 + 10a3z9 + 4az9 + 8a6z8 + 7a4z8 + 3a2z8 + 4z8 + 6a7z7−11a5z7−25a3z7−5az7 + 3z7a−1 + 3a8z6−21a6z6−28a4z6−11a2z6 + z6a−2−6z6 + a9z5−13a7z5 + 7a5z5 + 28a3z5−az5−8z5a−1−5a8z4 + 26a6z4 + 39a4z4 + 7a2z4−3z4a−2−4z4−2a9z3 + 10a7z3 + 6a5z3−14a3z3−2az3 + 6z3a−1−12a6z2−20a4z2−5a2z2 + 3z2a−2 + 6z2−3a7z−3a5z + a3z−za−1 + 2a6 + 4a4 + a2−a−2−1 |
| The A2 invariant | Data:K11a331/QuantumInvariant/A2/1,0 |
| The G2 invariant | Data:K11a331/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["K11a331"];
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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]=
| 2t3−11t2 + 27t−35 + 27t−1−11t−2 + 2t−3 |
In[5]:=
| Conway[K][z]
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Out[5]=
| 2z6 + z4 + z2 + 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]=
| { 115, -2 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| q3−3q2 + 7q−12 + 16q−1−18q−2 + 19q−3−16q−4 + 12q−5−7q−6 + 3q−7−q−8 |
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]=
| −z4a6−2z2a6−2a6 + z6a4 + 3z4a4 + 6z2a4 + 4a4 + z6a2 + z4a2−z2a2−a2−2z4−3z2−1 + z2a−2 + a−2 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| 2a4z10 + 2a2z10 + 6a5z9 + 10a3z9 + 4az9 + 8a6z8 + 7a4z8 + 3a2z8 + 4z8 + 6a7z7−11a5z7−25a3z7−5az7 + 3z7a−1 + 3a8z6−21a6z6−28a4z6−11a2z6 + z6a−2−6z6 + a9z5−13a7z5 + 7a5z5 + 28a3z5−az5−8z5a−1−5a8z4 + 26a6z4 + 39a4z4 + 7a2z4−3z4a−2−4z4−2a9z3 + 10a7z3 + 6a5z3−14a3z3−2az3 + 6z3a−1−12a6z2−20a4z2−5a2z2 + 3z2a−2 + 6z2−3a7z−3a5z + a3z−za−1 + 2a6 + 4a4 + a2−a−2−1 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {10_121, K11a41, K11a183, K11a198,}
Same Jones Polynomial (up to mirroring,
):
{K11a3, K11a51,}
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["K11a331"];
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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]=
| { 2t3−11t2 + 27t−35 + 27t−1−11t−2 + 2t−3, q3−3q2 + 7q−12 + 16q−1−18q−2 + 19q−3−16q−4 + 12q−5−7q−6 + 3q−7−q−8 } |
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]=
| {10_121, K11a41, K11a183, K11a198,} |
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]=
| {K11a3, K11a51,} |
[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 K11a331. 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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