K11n121
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11n121's page at Knotilus! Visit K11n121's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X4251 X10,3,11,4 X5,16,6,17 X7,12,8,13 X18,9,19,10 X2,11,3,12 X13,20,14,21 X15,6,16,7 X22,18,1,17 X8,19,9,20 X21,14,22,15 |
| Gauss code | 1, -6, 2, -1, -3, 8, -4, -10, 5, -2, 6, 4, -7, 11, -8, 3, 9, -5, 10, 7, -11, -9 |
| Dowker-Thistlethwaite code | 4 10 -16 -12 18 2 -20 -6 22 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 + 6t2−10t + 11−10t−1 + 6t−2−t−3 |
| Conway polynomial | −z6 + 5z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 45, -4 } |
| Jones polynomial | 1−3q−1 + 5q−2−6q−3 + 8q−4−7q−5 + 7q−6−5q−7 + 2q−8−q−9 |
| HOMFLY-PT polynomial (db, data sources) | −z2a8−2a8 + 2z4a6 + 5z2a6 + 2a6−z6a4−3z4a4−z2a4 + a4 + z4a2 + 2z2a2 |
| Kauffman polynomial (db, data sources) | z3a11−za11 + 2z4a10−z2a10 + 4z5a9−5z3a9 + 4za9 + z8a8−z6a8 + 2z4a8 + 2z2a8−2a8 + z9a7−2z7a7 + 6z5a7−10z3a7 + 6za7 + 4z8a6−11z6a6 + 9z4a6−2z2a6−2a6 + z9a5 + z7a5−8z5a5 + 3z3a5 + za5 + 3z8a4−9z6a4 + 6z4a4−3z2a4 + a4 + 3z7a3−10z5a3 + 7z3a3 + z6a2−3z4a2 + 2z2a2 |
| The A2 invariant | Data:K11n121/QuantumInvariant/A2/1,0 |
| The G2 invariant | Data:K11n121/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["K11n121"];
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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 + 6t2−10t + 11−10t−1 + 6t−2−t−3 |
In[5]:=
| Conway[K][z]
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Out[5]=
| −z6 + 5z2 + 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]=
| { 45, -4 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| 1−3q−1 + 5q−2−6q−3 + 8q−4−7q−5 + 7q−6−5q−7 + 2q−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]=
| −z2a8−2a8 + 2z4a6 + 5z2a6 + 2a6−z6a4−3z4a4−z2a4 + a4 + z4a2 + 2z2a2 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| z3a11−za11 + 2z4a10−z2a10 + 4z5a9−5z3a9 + 4za9 + z8a8−z6a8 + 2z4a8 + 2z2a8−2a8 + z9a7−2z7a7 + 6z5a7−10z3a7 + 6za7 + 4z8a6−11z6a6 + 9z4a6−2z2a6−2a6 + z9a5 + z7a5−8z5a5 + 3z3a5 + za5 + 3z8a4−9z6a4 + 6z4a4−3z2a4 + a4 + 3z7a3−10z5a3 + 7z3a3 + z6a2−3z4a2 + 2z2a2 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {K11n14,}
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["K11n121"];
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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 + 6t2−10t + 11−10t−1 + 6t−2−t−3, 1−3q−1 + 5q−2−6q−3 + 8q−4−7q−5 + 7q−6−5q−7 + 2q−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]=
| {K11n14,} |
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 K11n121. 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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