K11a282
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a282's page at Knotilus! Visit K11a282's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X10,4,11,3 X16,5,17,6 X14,8,15,7 X4,10,5,9 X18,11,19,12 X20,13,21,14 X22,16,1,15 X2,17,3,18 X12,19,13,20 X8,21,9,22 |
| Gauss code | 1, -9, 2, -5, 3, -1, 4, -11, 5, -2, 6, -10, 7, -4, 8, -3, 9, -6, 10, -7, 11, -8 |
| Dowker-Thistlethwaite code | 6 10 16 14 4 18 20 22 2 12 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 + 6t3−16t2 + 26t−29 + 26t−1−16t−2 + 6t−3−t−4 |
| Conway polynomial | −z8−2z6 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 127, -2 } |
| Jones polynomial | −q4 + 4q3−8q2 + 13q−17 + 20q−1−20q−2 + 18q−3−13q−4 + 8q−5−4q−6 + q−7 |
| HOMFLY-PT polynomial (db, data sources) | −a2z8 + a4z6−5a2z6 + 2z6 + 3a4z4−9a2z4−z4a−2 + 7z4 + 2a4z2−6a2z2−2z2a−2 + 6z2 + 1 |
| Kauffman polynomial (db, data sources) | 3a2z10 + 3z10 + 9a3z9 + 15az9 + 6z9a−1 + 12a4z8 + 10a2z8 + 4z8a−2 + 2z8 + 11a5z7−14a3z7−46az7−20z7a−1 + z7a−3 + 8a6z6−20a4z6−47a2z6−14z6a−2−33z6 + 4a7z5−13a5z5 + a3z5 + 39az5 + 18z5a−1−3z5a−3 + a8z4−7a6z4 + 10a4z4 + 45a2z4 + 14z4a−2 + 41z4−2a7z3 + 3a5z3 + 3a3z3−9az3−5z3a−1 + 2z3a−3 + a6z2−2a4z2−12a2z2−5z2a−2−14z2 + 1 |
| The A2 invariant | q20−2q18 + 2q16−2q14−q12 + 3q10−3q8 + 5q6−2q4 + q2 + 1−3q−2 + 3q−4−q−6 + q−8 + q−10−q−12 |
| The G2 invariant | Data:K11a282/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["K11a282"];
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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 + 6t3−16t2 + 26t−29 + 26t−1−16t−2 + 6t−3−t−4 |
In[5]:=
| Conway[K][z]
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Out[5]=
| −z8−2z6 + 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]=
| { 127, -2 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| −q4 + 4q3−8q2 + 13q−17 + 20q−1−20q−2 + 18q−3−13q−4 + 8q−5−4q−6 + q−7 |
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]=
| −a2z8 + a4z6−5a2z6 + 2z6 + 3a4z4−9a2z4−z4a−2 + 7z4 + 2a4z2−6a2z2−2z2a−2 + 6z2 + 1 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| 3a2z10 + 3z10 + 9a3z9 + 15az9 + 6z9a−1 + 12a4z8 + 10a2z8 + 4z8a−2 + 2z8 + 11a5z7−14a3z7−46az7−20z7a−1 + z7a−3 + 8a6z6−20a4z6−47a2z6−14z6a−2−33z6 + 4a7z5−13a5z5 + a3z5 + 39az5 + 18z5a−1−3z5a−3 + a8z4−7a6z4 + 10a4z4 + 45a2z4 + 14z4a−2 + 41z4−2a7z3 + 3a5z3 + 3a3z3−9az3−5z3a−1 + 2z3a−3 + a6z2−2a4z2−12a2z2−5z2a−2−14z2 + 1 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {K11a81,}
Same Jones Polynomial (up to mirroring,
):
{K11a81,}
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["K11a282"];
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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 + 6t3−16t2 + 26t−29 + 26t−1−16t−2 + 6t−3−t−4, −q4 + 4q3−8q2 + 13q−17 + 20q−1−20q−2 + 18q−3−13q−4 + 8q−5−4q−6 + q−7 } |
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]=
| {K11a81,} |
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]=
| {K11a81,} |
[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 K11a282. 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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