K11a122
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a122's page at Knotilus! Visit K11a122's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X4251 X10,3,11,4 X14,6,15,5 X18,7,19,8 X16,9,17,10 X2,11,3,12 X20,13,21,14 X22,16,1,15 X8,17,9,18 X12,19,13,20 X6,21,7,22 |
| Gauss code | 1, -6, 2, -1, 3, -11, 4, -9, 5, -2, 6, -10, 7, -3, 8, -5, 9, -4, 10, -7, 11, -8 |
| Dowker-Thistlethwaite code | 4 10 14 18 16 2 20 22 8 12 6 |
| 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 | 2t3−12t2 + 30t−39 + 30t−1−12t−2 + 2t−3 |
| Conway polynomial | 2z6 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 127, -2 } |
| Jones polynomial | −q2 + 4q−8 + 14q−1−18q−2 + 21q−3−20q−4 + 17q−5−13q−6 + 7q−7−3q−8 + q−9 |
| HOMFLY-PT polynomial (db, data sources) | z2a8 + a8−2z4a6−3z2a6−2a6 + z6a4 + z4a4 + z6a2 + 2z4a2 + 3z2a2 + 2a2−z4−z2 |
| Kauffman polynomial (db, data sources) | z6a10−3z4a10 + 2z2a10 + 3z7a9−8z5a9 + 6z3a9−2za9 + 5z8a8−12z6a8 + 9z4a8−4z2a8 + a8 + 5z9a7−9z7a7 + 4z5a7−2za7 + 2z10a6 + 7z8a6−26z6a6 + 28z4a6−13z2a6 + 2a6 + 11z9a5−23z7a5 + 20z5a5−9z3a5 + 2za5 + 2z10a4 + 10z8a4−27z6a4 + 23z4a4−6z2a4 + 6z9a3−4z7a3−3z5a3 + z3a3 + 2za3 + 8z8a2−10z6a2 + z4a2 + 3z2a2−2a2 + 7z7a−10z5a + 3z3a + 4z6−6z4 + 2z2 + z5a−1−z3a−1 |
| The A2 invariant | Data:K11a122/QuantumInvariant/A2/1,0 |
| The G2 invariant | Data:K11a122/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["K11a122"];
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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]=
| 2t3−12t2 + 30t−39 + 30t−1−12t−2 + 2t−3 |
In[5]:=
| Conway[K][z]
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Out[5]=
| 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]=
| −q2 + 4q−8 + 14q−1−18q−2 + 21q−3−20q−4 + 17q−5−13q−6 + 7q−7−3q−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 + a8−2z4a6−3z2a6−2a6 + z6a4 + z4a4 + z6a2 + 2z4a2 + 3z2a2 + 2a2−z4−z2 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| z6a10−3z4a10 + 2z2a10 + 3z7a9−8z5a9 + 6z3a9−2za9 + 5z8a8−12z6a8 + 9z4a8−4z2a8 + a8 + 5z9a7−9z7a7 + 4z5a7−2za7 + 2z10a6 + 7z8a6−26z6a6 + 28z4a6−13z2a6 + 2a6 + 11z9a5−23z7a5 + 20z5a5−9z3a5 + 2za5 + 2z10a4 + 10z8a4−27z6a4 + 23z4a4−6z2a4 + 6z9a3−4z7a3−3z5a3 + z3a3 + 2za3 + 8z8a2−10z6a2 + z4a2 + 3z2a2−2a2 + 7z7a−10z5a + 3z3a + 4z6−6z4 + 2z2 + z5a−1−z3a−1 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {K11a1, K11a149,}
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["K11a122"];
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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]=
| { 2t3−12t2 + 30t−39 + 30t−1−12t−2 + 2t−3, −q2 + 4q−8 + 14q−1−18q−2 + 21q−3−20q−4 + 17q−5−13q−6 + 7q−7−3q−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]=
| {K11a1, K11a149,} |
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 K11a122. 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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