K11a330
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a330's page at Knotilus! Visit K11a330's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X12,4,13,3 X18,5,19,6 X22,8,1,7 X16,9,17,10 X4,12,5,11 X20,13,21,14 X8,15,9,16 X10,17,11,18 X2,19,3,20 X14,21,15,22 |
| Gauss code | 1, -10, 2, -6, 3, -1, 4, -8, 5, -9, 6, -2, 7, -11, 8, -5, 9, -3, 10, -7, 11, -4 |
| Dowker-Thistlethwaite code | 6 12 18 22 16 4 20 8 10 2 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 + 12t2−17t + 19−17t−1 + 12t−2−5t−3 + t−4 |
| Conway polynomial | z8 + 3z6 + 2z4 + 2z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 89, -4 } |
| Jones polynomial | q2−3q + 6−9q−1 + 12q−2−13q−3 + 14q−4−12q−5 + 9q−6−6q−7 + 3q−8−q−9 |
| HOMFLY-PT polynomial (db, data sources) | a4z8−a6z6 + 6a4z6−2a2z6−4a6z4 + 14a4z4−9a2z4 + z4−5a6z2 + 16a4z2−12a2z2 + 3z2−3a6 + 7a4−5a2 + 2 |
| Kauffman polynomial (db, data sources) | z3a11 + 3z4a10 + 6z5a9−4z3a9 + za9 + 9z6a8−12z4a8 + 3z2a8 + 11z7a7−22z5a7 + 9z3a7−2za7 + 11z8a6−30z6a6 + 23z4a6−12z2a6 + 3a6 + 7z9a5−16z7a5−3z5a5 + 13z3a5−4za5 + 2z10a4 + 7z8a4−52z6a4 + 72z4a4−35z2a4 + 7a4 + 10z9a3−42z7a3 + 49z5a3−14z3a3 + 2z10a2−3z8a2−18z6a2 + 43z4a2−27z2a2 + 5a2 + 3z9a−15z7a + 24z5a−13z3a + za + z8−5z6 + 9z4−7z2 + 2 |
| The A2 invariant | −q26 + q24−2q22−q16 + 4q14−q12 + 3q10−q6 + q4−2q2 + 1 + q−6 |
| The G2 invariant | Data:K11a330/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["K11a330"];
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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 + 12t2−17t + 19−17t−1 + 12t−2−5t−3 + t−4 |
In[5]:=
| Conway[K][z]
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Out[5]=
| z8 + 3z6 + 2z4 + 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]=
| { 89, -4 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| q2−3q + 6−9q−1 + 12q−2−13q−3 + 14q−4−12q−5 + 9q−6−6q−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]=
| a4z8−a6z6 + 6a4z6−2a2z6−4a6z4 + 14a4z4−9a2z4 + z4−5a6z2 + 16a4z2−12a2z2 + 3z2−3a6 + 7a4−5a2 + 2 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| z3a11 + 3z4a10 + 6z5a9−4z3a9 + za9 + 9z6a8−12z4a8 + 3z2a8 + 11z7a7−22z5a7 + 9z3a7−2za7 + 11z8a6−30z6a6 + 23z4a6−12z2a6 + 3a6 + 7z9a5−16z7a5−3z5a5 + 13z3a5−4za5 + 2z10a4 + 7z8a4−52z6a4 + 72z4a4−35z2a4 + 7a4 + 10z9a3−42z7a3 + 49z5a3−14z3a3 + 2z10a2−3z8a2−18z6a2 + 43z4a2−27z2a2 + 5a2 + 3z9a−15z7a + 24z5a−13z3a + za + z8−5z6 + 9z4−7z2 + 2 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {K11a40,}
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["K11a330"];
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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 + 12t2−17t + 19−17t−1 + 12t−2−5t−3 + t−4, q2−3q + 6−9q−1 + 12q−2−13q−3 + 14q−4−12q−5 + 9q−6−6q−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]=
| {K11a40,} |
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 = -4 is the signature of K11a330. 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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