K11a2
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a2's page at Knotilus! Visit K11a2's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X4251 X8394 X10,6,11,5 X14,8,15,7 X2,9,3,10 X18,12,19,11 X6,14,7,13 X20,16,21,15 X12,18,13,17 X22,20,1,19 X16,22,17,21 |
| Gauss code | 1, -5, 2, -1, 3, -7, 4, -2, 5, -3, 6, -9, 7, -4, 8, -11, 9, -6, 10, -8, 11, -10 |
| Dowker-Thistlethwaite code | 4 8 10 14 2 18 6 20 12 22 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 | −3t3 + 15t2−31t + 39−31t−1 + 15t−2−3t−3 |
| Conway polynomial | −3z6−3z4 + 2z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 137, 4 } |
| Jones polynomial | −q11 + 4q10−9q9 + 15q8−20q7 + 22q6−22q5 + 19q4−13q3 + 8q2−3q + 1 |
| HOMFLY-PT polynomial (db, data sources) | −z6a−4−2z6a−6 + z4a−2−z4a−4−6z4a−6 + 3z4a−8 + 2z2a−2 + 2z2a−4−7z2a−6 + 6z2a−8−z2a−10 + a−2 + 2a−4−4a−6 + 3a−8−a−10 |
| Kauffman polynomial (db, data sources) | z10a−6 + z10a−8 + 4z9a−5 + 9z9a−7 + 5z9a−9 + 5z8a−4 + 16z8a−6 + 20z8a−8 + 9z8a−10 + 3z7a−3 + z7a−5 + 10z7a−9 + 8z7a−11 + z6a−2−10z6a−4−42z6a−6−45z6a−8−10z6a−10 + 4z6a−12−7z5a−3−17z5a−5−33z5a−7−36z5a−9−12z5a−11 + z5a−13−3z4a−2 + 7z4a−4 + 38z4a−6 + 35z4a−8 + 2z4a−10−5z4a−12 + 5z3a−3 + 17z3a−5 + 33z3a−7 + 30z3a−9 + 8z3a−11−z3a−13 + 3z2a−2−4z2a−4−18z2a−6−14z2a−8−z2a−10 + 2z2a−12−za−3−6za−5−10za−7−8za−9−3za−11−a−2 + 2a−4 + 4a−6 + 3a−8 + a−10 |
| The A2 invariant | Data:K11a2/QuantumInvariant/A2/1,0 |
| The G2 invariant | Data:K11a2/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["K11a2"];
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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]=
| −3t3 + 15t2−31t + 39−31t−1 + 15t−2−3t−3 |
In[5]:=
| Conway[K][z]
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Out[5]=
| −3z6−3z4 + 2z2 + 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]=
| { 137, 4 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| −q11 + 4q10−9q9 + 15q8−20q7 + 22q6−22q5 + 19q4−13q3 + 8q2−3q + 1 |
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]=
| −z6a−4−2z6a−6 + z4a−2−z4a−4−6z4a−6 + 3z4a−8 + 2z2a−2 + 2z2a−4−7z2a−6 + 6z2a−8−z2a−10 + a−2 + 2a−4−4a−6 + 3a−8−a−10 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| z10a−6 + z10a−8 + 4z9a−5 + 9z9a−7 + 5z9a−9 + 5z8a−4 + 16z8a−6 + 20z8a−8 + 9z8a−10 + 3z7a−3 + z7a−5 + 10z7a−9 + 8z7a−11 + z6a−2−10z6a−4−42z6a−6−45z6a−8−10z6a−10 + 4z6a−12−7z5a−3−17z5a−5−33z5a−7−36z5a−9−12z5a−11 + z5a−13−3z4a−2 + 7z4a−4 + 38z4a−6 + 35z4a−8 + 2z4a−10−5z4a−12 + 5z3a−3 + 17z3a−5 + 33z3a−7 + 30z3a−9 + 8z3a−11−z3a−13 + 3z2a−2−4z2a−4−18z2a−6−14z2a−8−z2a−10 + 2z2a−12−za−3−6za−5−10za−7−8za−9−3za−11−a−2 + 2a−4 + 4a−6 + 3a−8 + a−10 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {K11a116,}
Same Jones Polynomial (up to mirroring,
):
{K11a116,}
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["K11a2"];
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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]=
| { −3t3 + 15t2−31t + 39−31t−1 + 15t−2−3t−3, −q11 + 4q10−9q9 + 15q8−20q7 + 22q6−22q5 + 19q4−13q3 + 8q2−3q + 1 } |
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]=
| {K11a116,} |
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]=
| {K11a116,} |
[edit] Vassiliev invariants
| V2 and V3: | (2, 4) |
| 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 = 4 is the signature of K11a2. 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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