K11n159
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11n159's page at Knotilus! Visit K11n159's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X10,3,11,4 X12,6,13,5 X7,18,8,19 X9,20,10,21 X16,11,17,12 X22,13,1,14 X4,16,5,15 X2,17,3,18 X19,8,20,9 X14,21,15,22 |
| Gauss code | 1, -9, 2, -8, 3, -1, -4, 10, -5, -2, 6, -3, 7, -11, 8, -6, 9, 4, -10, 5, 11, -7 |
| Dowker-Thistlethwaite code | 6 10 12 -18 -20 16 22 4 2 -8 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 | t3−6t2 + 17t−23 + 17t−1−6t−2 + t−3 |
| Conway polynomial | z6 + 2z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 71, -2 } |
| Jones polynomial | −1 + 5q−1−8q−2 + 11q−3−12q−4 + 12q−5−10q−6 + 7q−7−4q−8 + q−9 |
| HOMFLY-PT polynomial (db, data sources) | z2a8−2z4a6−3z2a6−a6 + z6a4 + 3z4a4 + 4z2a4 + a4−z4a2 + a2 |
| Kauffman polynomial (db, data sources) | z6a10−2z4a10 + z2a10 + 4z7a9−11z5a9 + 7z3a9 + 5z8a8−12z6a8 + 4z4a8 + z2a8 + 2z9a7 + 4z7a7−21z5a7 + 13z3a7−2za7 + 9z8a6−21z6a6 + 13z4a6−5z2a6 + a6 + 2z9a5 + 2z7a5−9z5a5 + 6z3a5−2za5 + 4z8a4−8z6a4 + 12z4a4−6z2a4 + a4 + 2z7a3 + z5a3 + z3a3 + 5z4a2−z2a2−a2 + z3a |
| The A2 invariant | q28−q26−2q24 + 2q22−2q20 + q18 + q16−2q14 + 2q12−2q10 + 3q8 + q6−q4 + 3q2−1 |
| The G2 invariant | Data:K11n159/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["K11n159"];
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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]=
| t3−6t2 + 17t−23 + 17t−1−6t−2 + t−3 |
In[5]:=
| Conway[K][z]
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Out[5]=
| z6 + 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]=
| { 71, -2 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| −1 + 5q−1−8q−2 + 11q−3−12q−4 + 12q−5−10q−6 + 7q−7−4q−8 + q−9 |
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]=
| z2a8−2z4a6−3z2a6−a6 + z6a4 + 3z4a4 + 4z2a4 + a4−z4a2 + a2 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| z6a10−2z4a10 + z2a10 + 4z7a9−11z5a9 + 7z3a9 + 5z8a8−12z6a8 + 4z4a8 + z2a8 + 2z9a7 + 4z7a7−21z5a7 + 13z3a7−2za7 + 9z8a6−21z6a6 + 13z4a6−5z2a6 + a6 + 2z9a5 + 2z7a5−9z5a5 + 6z3a5−2za5 + 4z8a4−8z6a4 + 12z4a4−6z2a4 + a4 + 2z7a3 + z5a3 + z3a3 + 5z4a2−z2a2−a2 + z3a |
[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["K11n159"];
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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]=
| { t3−6t2 + 17t−23 + 17t−1−6t−2 + t−3, −1 + 5q−1−8q−2 + 11q−3−12q−4 + 12q−5−10q−6 + 7q−7−4q−8 + q−9 } |
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 = -2 is the signature of K11n159. 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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