K11a67
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a67's page at Knotilus! Visit K11a67's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X4251 X8394 X16,5,17,6 X12,8,13,7 X2,9,3,10 X18,12,19,11 X22,13,1,14 X20,15,21,16 X10,18,11,17 X6,19,7,20 X14,21,15,22 |
| Gauss code | 1, -5, 2, -1, 3, -10, 4, -2, 5, -9, 6, -4, 7, -11, 8, -3, 9, -6, 10, -8, 11, -7 |
| Dowker-Thistlethwaite code | 4 8 16 12 2 18 22 20 10 6 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 | −2t3 + 12t2−29t + 39−29t−1 + 12t−2−2t−3 |
| Conway polynomial | −2z6 + z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 125, 0 } |
| Jones polynomial | q4−4q3 + 9q2−14q + 18−20q−1 + 20q−2−16q−3 + 12q−4−7q−5 + 3q−6−q−7 |
| HOMFLY-PT polynomial (db, data sources) | −z2a6−a6 + 2z4a4 + 3z2a4 + a4−z6a2−z4a2 + z2a2 + 2a2−z6−2z4−3z2−2 + z4a−2 + z2a−2 + a−2 |
| Kauffman polynomial (db, data sources) | 2a4z10 + 2a2z10 + 4a5z9 + 11a3z9 + 7az9 + 3a6z8 + 4a4z8 + 13a2z8 + 12z8 + a7z7−11a5z7−25a3z7 + 13z7a−1−11a6z6−27a4z6−40a2z6 + 9z6a−2−15z6−4a7z5 + 5a5z5 + 7a3z5−24az5−18z5a−1 + 4z5a−3 + 13a6z4 + 29a4z4 + 24a2z4−8z4a−2 + z4a−4−z4 + 5a7z3 + 5a5z3 + 8a3z3 + 18az3 + 9z3a−1−z3a−3−6a6z2−9a4z2 + 3z2a−2 + 6z2−2a7z−3a5z−3a3z−4az−2za−1 + a6 + a4−2a2−a−2−2 |
| The A2 invariant | Data:K11a67/QuantumInvariant/A2/1,0 |
| The G2 invariant | Data:K11a67/QuantumInvariant/G2/1,0 |
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["K11a67"];
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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 + 12t2−29t + 39−29t−1 + 12t−2−2t−3 |
In[5]:=
| Conway[K][z]
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Out[5]=
| −2z6 + z2 + 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]=
| { 125, 0 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| q4−4q3 + 9q2−14q + 18−20q−1 + 20q−2−16q−3 + 12q−4−7q−5 + 3q−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]=
| −z2a6−a6 + 2z4a4 + 3z2a4 + a4−z6a2−z4a2 + z2a2 + 2a2−z6−2z4−3z2−2 + z4a−2 + z2a−2 + a−2 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| 2a4z10 + 2a2z10 + 4a5z9 + 11a3z9 + 7az9 + 3a6z8 + 4a4z8 + 13a2z8 + 12z8 + a7z7−11a5z7−25a3z7 + 13z7a−1−11a6z6−27a4z6−40a2z6 + 9z6a−2−15z6−4a7z5 + 5a5z5 + 7a3z5−24az5−18z5a−1 + 4z5a−3 + 13a6z4 + 29a4z4 + 24a2z4−8z4a−2 + z4a−4−z4 + 5a7z3 + 5a5z3 + 8a3z3 + 18az3 + 9z3a−1−z3a−3−6a6z2−9a4z2 + 3z2a−2 + 6z2−2a7z−3a5z−3a3z−4az−2za−1 + a6 + a4−2a2−a−2−2 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {K11a104, K11a168,}
Same Jones Polynomial (up to mirroring,
):
{K11a317,}
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["K11a67"];
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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 + 12t2−29t + 39−29t−1 + 12t−2−2t−3, q4−4q3 + 9q2−14q + 18−20q−1 + 20q−2−16q−3 + 12q−4−7q−5 + 3q−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]=
| {K11a104, K11a168,} |
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]=
| {K11a317,} |
[edit] Vassiliev invariants
| V2 and V3: | (1, -3) |
| V2,1 through V6,9: |
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V2,1 through V6,9 were provided by Petr Dunin-Barkowski <barkovs@itep.ru>, Andrey Smirnov <asmirnov@itep.ru>, and Alexei Sleptsov <sleptsov@itep.ru> and uploaded on October 2010 by User:Drorbn. Note that they are normalized differently than V2 and V3.
[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 = 0 is the signature of K11a67. 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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