K11a216
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a216's page at Knotilus! Visit K11a216's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X4251 X12,4,13,3 X18,6,19,5 X14,7,15,8 X20,10,21,9 X2,12,3,11 X22,13,1,14 X8,15,9,16 X10,18,11,17 X6,20,7,19 X16,21,17,22 |
| Gauss code | 1, -6, 2, -1, 3, -10, 4, -8, 5, -9, 6, -2, 7, -4, 8, -11, 9, -3, 10, -5, 11, -7 |
| Dowker-Thistlethwaite code | 4 12 18 14 20 2 22 8 10 6 16 |
| 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 + 6t3−17t2 + 31t−37 + 31t−1−17t−2 + 6t−3−t−4 |
| Conway polynomial | −z8−2z6−z4 + z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 147, 2 } |
| Jones polynomial | −q8 + 4q7−9q6 + 15q5−21q4 + 24q3−23q2 + 21q−15 + 9q−1−4q−2 + q−3 |
| HOMFLY-PT polynomial (db, data sources) | −z8a−2−5z6a−2 + 2z6a−4 + z6−10z4a−2 + 7z4a−4−z4a−6 + 3z4−8z2a−2 + 8z2a−4−2z2a−6 + 3z2−a−2 + 2a−4−a−6 + 1 |
| Kauffman polynomial (db, data sources) | 2z10a−2 + 2z10a−4 + 6z9a−1 + 13z9a−3 + 7z9a−5 + 15z8a−2 + 18z8a−4 + 10z8a−6 + 7z8 + 4az7−4z7a−1−16z7a−3 + 8z7a−7 + a2z6−44z6a−2−47z6a−4−15z6a−6 + 4z6a−8−15z6−9az5−13z5a−1−9z5a−3−18z5a−5−12z5a−7 + z5a−9−2a2z4 + 38z4a−2 + 41z4a−4 + 10z4a−6−5z4a−8 + 10z4 + 6az3 + 12z3a−1 + 16z3a−3 + 18z3a−5 + 7z3a−7−z3a−9 + a2z2−15z2a−2−15z2a−4−4z2a−6 + z2a−8−4z2−az−3za−1−4za−3−4za−5−2za−7 + a−2 + 2a−4 + a−6 + 1 |
| The A2 invariant | q8−2q6 + 3q4−2q2−1 + 4q−2−4q−4 + 6q−6−2q−8 + q−10 + q−12−4q−14 + 4q−16−2q−18 + q−22−q−24 |
| The G2 invariant | q46−3q44 + 8q42−16q40 + 22q38−25q36 + 14q34 + 18q32−66q30 + 129q28−176q26 + 173q24−98q22−67q20 + 290q18−494q16 + 587q14−481q12 + 158q10 + 304q8−746q6 + 998q4−914q2 + 492 + 127q−2−723q−4 + 1027q−6−919q−8 + 449q−10 + 188q−12−688q−14 + 841q−16−570q−18−12q−20 + 643q−22−1038q−24 + 998q−26−517q−28−239q−30 + 989q−32−1425q−34 + 1393q−36−879q−38 + 60q−40 + 769q−42−1323q−44 + 1389q−46−970q−48 + 253q−50 + 481q−52−920q−54 + 915q−56−499q−58−114q−60 + 636q−62−836q−64 + 614q−66−87q−68−512q−70 + 930q−72−980q−74 + 679q−76−154q−78−393q−80 + 751q−82−847q−84 + 677q−86−341q−88−17q−90 + 288q−92−413q−94 + 398q−96−287q−98 + 143q−100−9q−102−82q−104 + 116q−106−114q−108 + 83q−110−45q−112 + 16q−114 + 7q−116−16q−118 + 16q−120−13q−122 + 7q−124−3q−126 + q−128 |
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["K11a216"];
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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 + 6t3−17t2 + 31t−37 + 31t−1−17t−2 + 6t−3−t−4 |
In[5]:=
| Conway[K][z]
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Out[5]=
| −z8−2z6−z4 + 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]=
| { 147, 2 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| −q8 + 4q7−9q6 + 15q5−21q4 + 24q3−23q2 + 21q−15 + 9q−1−4q−2 + q−3 |
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]=
| −z8a−2−5z6a−2 + 2z6a−4 + z6−10z4a−2 + 7z4a−4−z4a−6 + 3z4−8z2a−2 + 8z2a−4−2z2a−6 + 3z2−a−2 + 2a−4−a−6 + 1 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| 2z10a−2 + 2z10a−4 + 6z9a−1 + 13z9a−3 + 7z9a−5 + 15z8a−2 + 18z8a−4 + 10z8a−6 + 7z8 + 4az7−4z7a−1−16z7a−3 + 8z7a−7 + a2z6−44z6a−2−47z6a−4−15z6a−6 + 4z6a−8−15z6−9az5−13z5a−1−9z5a−3−18z5a−5−12z5a−7 + z5a−9−2a2z4 + 38z4a−2 + 41z4a−4 + 10z4a−6−5z4a−8 + 10z4 + 6az3 + 12z3a−1 + 16z3a−3 + 18z3a−5 + 7z3a−7−z3a−9 + a2z2−15z2a−2−15z2a−4−4z2a−6 + z2a−8−4z2−az−3za−1−4za−3−4za−5−2za−7 + a−2 + 2a−4 + a−6 + 1 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {K11a196, K11a286,}
Same Jones Polynomial (up to mirroring,
):
{K11a196,}
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["K11a216"];
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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 + 6t3−17t2 + 31t−37 + 31t−1−17t−2 + 6t−3−t−4, −q8 + 4q7−9q6 + 15q5−21q4 + 24q3−23q2 + 21q−15 + 9q−1−4q−2 + q−3 } |
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]=
| {K11a196, K11a286,} |
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]=
| {K11a196,} |
[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 K11a216. 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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