K11a86
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a86's page at Knotilus! Visit K11a86's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X4251 X10,3,11,4 X12,6,13,5 X16,8,17,7 X18,10,19,9 X2,11,3,12 X20,13,21,14 X6,16,7,15 X8,18,9,17 X22,19,1,20 X14,21,15,22 |
| Gauss code | 1, -6, 2, -1, 3, -8, 4, -9, 5, -2, 6, -3, 7, -11, 8, -4, 9, -5, 10, -7, 11, -10 |
| Dowker-Thistlethwaite code | 4 10 12 16 18 2 20 6 8 22 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 | −t4 + 5t3−12t2 + 18t−19 + 18t−1−12t−2 + 5t−3−t−4 |
| Conway polynomial | −z8−3z6−2z4−z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 91, 2 } |
| Jones polynomial | q7−3q6 + 6q5−10q4 + 13q3−14q2 + 14q−12 + 9q−1−5q−2 + 3q−3−q−4 |
| HOMFLY-PT polynomial (db, data sources) | −z8a−2−6z6a−2 + z6a−4 + 2z6−a2z4−14z4a−2 + 4z4a−4 + 9z4−3a2z2−15z2a−2 + 5z2a−4 + 12z2−a2−5a−2 + 2a−4 + 5 |
| Kauffman polynomial (db, data sources) | z10a−2 + z10 + 3az9 + 7z9a−1 + 4z9a−3 + 3a2z8 + 9z8a−2 + 6z8a−4 + 6z8 + a3z7−9az7−20z7a−1−4z7a−3 + 6z7a−5−13a2z6−36z6a−2−9z6a−4 + 5z6a−6−35z6−4a3z5 + 3az5 + 14z5a−1−2z5a−3−6z5a−5 + 3z5a−7 + 17a2z4 + 45z4a−2 + 7z4a−4−5z4a−6 + z4a−8 + 49z4 + 4a3z3 + 5az3−2z3a−1 + z3a−3 + z3a−5−3z3a−7−8a2z2−26z2a−2−5z2a−4 + 2z2a−6−z2a−8−26z2−a3z−2az−za−1 + za−5 + za−7 + a2 + 5a−2 + 2a−4 + 5 |
| The A2 invariant | −q12 + q8 + 3q4−q2 + 1 + q−2−2q−4 + 3q−6−3q−8 + q−10−q−12−q−14 + 2q−16−q−18 + q−20 |
| The G2 invariant | q60−2q58 + 5q56−9q54 + 10q52−11q50 + 3q48 + 14q46−35q44 + 57q42−66q40 + 48q38−8q36−54q34 + 115q32−153q30 + 144q28−77q26−25q24 + 131q22−196q20 + 197q18−123q16 + 13q14 + 97q12−163q10 + 159q8−78q6−23q4 + 116q2−144 + 96q−2−2q−4−111q−6 + 188q−8−199q−10 + 135q−12−10q−14−126q−16 + 233q−18−263q−20 + 201q−22−81q−24−64q−26 + 176q−28−222q−30 + 186q−32−84q−34−29q−36 + 115q−38−137q−40 + 82q−42−82q−46 + 119q−48−98q−50 + 32q−52 + 51q−54−118q−56 + 147q−58−124q−60 + 63q−62 + 7q−64−72q−66 + 110q−68−116q−70 + 101q−72−58q−74 + 14q−76 + 30q−78−62q−80 + 71q−82−66q−84 + 48q−86−20q−88−4q−90 + 22q−92−30q−94 + 28q−96−20q−98 + 11q−100−2q−102−4q−104 + 5q−106−6q−108 + 4q−110−2q−112 + q−114 |
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["K11a86"];
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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 + 5t3−12t2 + 18t−19 + 18t−1−12t−2 + 5t−3−t−4 |
In[5]:=
| Conway[K][z]
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Out[5]=
| −z8−3z6−2z4−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]=
| { 91, 2 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| q7−3q6 + 6q5−10q4 + 13q3−14q2 + 14q−12 + 9q−1−5q−2 + 3q−3−q−4 |
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−2−6z6a−2 + z6a−4 + 2z6−a2z4−14z4a−2 + 4z4a−4 + 9z4−3a2z2−15z2a−2 + 5z2a−4 + 12z2−a2−5a−2 + 2a−4 + 5 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| z10a−2 + z10 + 3az9 + 7z9a−1 + 4z9a−3 + 3a2z8 + 9z8a−2 + 6z8a−4 + 6z8 + a3z7−9az7−20z7a−1−4z7a−3 + 6z7a−5−13a2z6−36z6a−2−9z6a−4 + 5z6a−6−35z6−4a3z5 + 3az5 + 14z5a−1−2z5a−3−6z5a−5 + 3z5a−7 + 17a2z4 + 45z4a−2 + 7z4a−4−5z4a−6 + z4a−8 + 49z4 + 4a3z3 + 5az3−2z3a−1 + z3a−3 + z3a−5−3z3a−7−8a2z2−26z2a−2−5z2a−4 + 2z2a−6−z2a−8−26z2−a3z−2az−za−1 + za−5 + za−7 + a2 + 5a−2 + 2a−4 + 5 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {}
Same Jones Polynomial (up to mirroring,
):
{K11a205,}
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["K11a86"];
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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 + 5t3−12t2 + 18t−19 + 18t−1−12t−2 + 5t−3−t−4, q7−3q6 + 6q5−10q4 + 13q3−14q2 + 14q−12 + 9q−1−5q−2 + 3q−3−q−4 } |
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]=
| {K11a205,} |
[edit] Vassiliev invariants
| V2 and V3: | (-1, -2) |
| 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 = 2 is the signature of K11a86. 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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