K11a325
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a325's page at Knotilus! Visit K11a325's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X12,3,13,4 X16,5,17,6 X22,8,1,7 X20,10,21,9 X18,11,19,12 X2,13,3,14 X10,15,11,16 X4,17,5,18 X14,19,15,20 X8,22,9,21 |
| Gauss code | 1, -7, 2, -9, 3, -1, 4, -11, 5, -8, 6, -2, 7, -10, 8, -3, 9, -6, 10, -5, 11, -4 |
| Dowker-Thistlethwaite code | 6 12 16 22 20 18 2 10 4 14 8 |
| 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 | −6t2 + 24t−35 + 24t−1−6t−2 |
| Conway polynomial | 1−6z4 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 95, -2 } |
| Jones polynomial | q3−3q2 + 6q−9 + 13q−1−15q−2 + 15q−3−13q−4 + 10q−5−6q−6 + 3q−7−q−8 |
| HOMFLY-PT polynomial (db, data sources) | −a8 + 3z2a6 + 2a6−2z4a4−z2a4−3z4a2−4z2a2−2a2−z4 + z2 + 2 + z2a−2 |
| Kauffman polynomial (db, data sources) | 2a4z10 + 2a2z10 + 4a5z9 + 9a3z9 + 5az9 + 4a6z8 + a2z8 + 5z8 + 4a7z7−8a5z7−32a3z7−17az7 + 3z7a−1 + 3a8z6−3a6z6−9a4z6−21a2z6 + z6a−2−17z6 + a9z5−5a7z5 + 10a5z5 + 45a3z5 + 20az5−9z5a−1−6a8z4−6a6z4 + 17a4z4 + 37a2z4−3z4a−2 + 17z4−2a9z3−2a7z3−6a5z3−21a3z3−11az3 + 4z3a−1 + 3a8z2 + 6a6z2−6a4z2−19a2z2 + z2a−2−9z2 + a9z + a7z + a5z + 3a3z + 2az−a8−2a6 + 2a2 + 2 |
| The A2 invariant | Data:K11a325/QuantumInvariant/A2/1,0 |
| The G2 invariant | Data:K11a325/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["K11a325"];
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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]=
| −6t2 + 24t−35 + 24t−1−6t−2 |
In[5]:=
| Conway[K][z]
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Out[5]=
| 1−6z4 |
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]=
| { 95, -2 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| q3−3q2 + 6q−9 + 13q−1−15q−2 + 15q−3−13q−4 + 10q−5−6q−6 + 3q−7−q−8 |
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]=
| −a8 + 3z2a6 + 2a6−2z4a4−z2a4−3z4a2−4z2a2−2a2−z4 + z2 + 2 + z2a−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 + 9a3z9 + 5az9 + 4a6z8 + a2z8 + 5z8 + 4a7z7−8a5z7−32a3z7−17az7 + 3z7a−1 + 3a8z6−3a6z6−9a4z6−21a2z6 + z6a−2−17z6 + a9z5−5a7z5 + 10a5z5 + 45a3z5 + 20az5−9z5a−1−6a8z4−6a6z4 + 17a4z4 + 37a2z4−3z4a−2 + 17z4−2a9z3−2a7z3−6a5z3−21a3z3−11az3 + 4z3a−1 + 3a8z2 + 6a6z2−6a4z2−19a2z2 + z2a−2−9z2 + a9z + a7z + a5z + 3a3z + 2az−a8−2a6 + 2a2 + 2 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {}
Same Jones Polynomial (up to mirroring,
):
{K11a7,}
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["K11a325"];
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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]=
| { −6t2 + 24t−35 + 24t−1−6t−2, q3−3q2 + 6q−9 + 13q−1−15q−2 + 15q−3−13q−4 + 10q−5−6q−6 + 3q−7−q−8 } |
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]=
| {K11a7,} |
[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 K11a325. 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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