K11a261
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a261's page at Knotilus! Visit K11a261's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X8394 X14,5,15,6 X16,8,17,7 X4,9,5,10 X18,11,19,12 X20,13,21,14 X2,15,3,16 X22,18,1,17 X12,19,13,20 X10,21,11,22 |
| Gauss code | 1, -8, 2, -5, 3, -1, 4, -2, 5, -11, 6, -10, 7, -3, 8, -4, 9, -6, 10, -7, 11, -9 |
| Dowker-Thistlethwaite code | 6 8 14 16 4 18 20 2 22 12 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 | t4−6t3 + 16t2−26t + 31−26t−1 + 16t−2−6t−3 + t−4 |
| Conway polynomial | z8 + 2z6 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 129, -4 } |
| Jones polynomial | −q + 4−7q−1 + 13q−2−17q−3 + 20q−4−21q−5 + 18q−6−14q−7 + 9q−8−4q−9 + q−10 |
| HOMFLY-PT polynomial (db, data sources) | z4a8 + 2z2a8 + a8−2z6a6−7z4a6−7z2a6−2a6 + z8a4 + 5z6a4 + 9z4a4 + 6z2a4−z6a2−3z4a2−z2a2 + 2a2 |
| Kauffman polynomial (db, data sources) | z4a12 + 4z5a11−z3a11 + 9z6a10−8z4a10 + 3z2a10 + 13z7a9−18z5a9 + 10z3a9−2za9 + 12z8a8−15z6a8 + 3z4a8−2z2a8 + a8 + 7z9a7 + z7a7−24z5a7 + 14z3a7−2za7 + 2z10a6 + 15z8a6−48z6a6 + 39z4a6−15z2a6 + 2a6 + 12z9a5−28z7a5 + 12z5a5 + 2za5 + 2z10a4 + 7z8a4−39z6a4 + 44z4a4−14z2a4 + 5z9a3−15z7a3 + 11z5a3−z3a3 + 2za3 + 4z8a2−15z6a2 + 17z4a2−4z2a2−2a2 + z7a−3z5a + 2z3a |
| The A2 invariant | q30−q28 + 2q24−3q22 + 3q20−2q18−q16 + q14−5q12 + 4q10−2q8 + 3q6 + 3q4−q2 + 2−q−2 |
| The G2 invariant | Data:K11a261/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["K11a261"];
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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 + 31−26t−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]=
| { 129, -4 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| −q + 4−7q−1 + 13q−2−17q−3 + 20q−4−21q−5 + 18q−6−14q−7 + 9q−8−4q−9 + q−10 |
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]=
| z4a8 + 2z2a8 + a8−2z6a6−7z4a6−7z2a6−2a6 + z8a4 + 5z6a4 + 9z4a4 + 6z2a4−z6a2−3z4a2−z2a2 + 2a2 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| z4a12 + 4z5a11−z3a11 + 9z6a10−8z4a10 + 3z2a10 + 13z7a9−18z5a9 + 10z3a9−2za9 + 12z8a8−15z6a8 + 3z4a8−2z2a8 + a8 + 7z9a7 + z7a7−24z5a7 + 14z3a7−2za7 + 2z10a6 + 15z8a6−48z6a6 + 39z4a6−15z2a6 + 2a6 + 12z9a5−28z7a5 + 12z5a5 + 2za5 + 2z10a4 + 7z8a4−39z6a4 + 44z4a4−14z2a4 + 5z9a3−15z7a3 + 11z5a3−z3a3 + 2za3 + 4z8a2−15z6a2 + 17z4a2−4z2a2−2a2 + z7a−3z5a + 2z3a |
[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["K11a261"];
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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 + 31−26t−1 + 16t−2−6t−3 + t−4, −q + 4−7q−1 + 13q−2−17q−3 + 20q−4−21q−5 + 18q−6−14q−7 + 9q−8−4q−9 + q−10 } |
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 = -4 is the signature of K11a261. 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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