K11a295
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a295's page at Knotilus! Visit K11a295's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X10,3,11,4 X16,5,17,6 X22,8,1,7 X18,9,19,10 X2,11,3,12 X20,13,21,14 X8,15,9,16 X4,17,5,18 X12,19,13,20 X14,21,15,22 |
| Gauss code | 1, -6, 2, -9, 3, -1, 4, -8, 5, -2, 6, -10, 7, -11, 8, -3, 9, -5, 10, -7, 11, -4 |
| Dowker-Thistlethwaite code | 6 10 16 22 18 2 20 8 4 12 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 | −3t3 + 14t2−24t + 27−24t−1 + 14t−2−3t−3 |
| Conway polynomial | −3z6−4z4 + 5z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 109, -4 } |
| Jones polynomial | 1−3q−1 + 7q−2−11q−3 + 15q−4−17q−5 + 18q−6−15q−7 + 11q−8−7q−9 + 3q−10−q−11 |
| HOMFLY-PT polynomial (db, data sources) | −z2a10−2a10 + 3z4a8 + 8z2a8 + 4a8−2z6a6−7z4a6−8z2a6−4a6−z6a4−z4a4 + 4z2a4 + 3a4 + z4a2 + 2z2a2 |
| Kauffman polynomial (db, data sources) | z5a13−2z3a13 + za13 + 3z6a12−5z4a12 + z2a12 + 5z7a11−8z5a11 + 3z3a11−2za11 + 6z8a10−11z6a10 + 10z4a10−7z2a10 + 2a10 + 5z9a9−8z7a9 + 5z5a9 + 2z3a9−za9 + 2z10a8 + 5z8a8−24z6a8 + 36z4a8−18z2a8 + 4a8 + 10z9a7−29z7a7 + 35z5a7−16z3a7 + 3za7 + 2z10a6 + 4z8a6−25z6a6 + 37z4a6−22z2a6 + 4a6 + 5z9a5−13z7a5 + 13z5a5−9z3a5 + za5 + 5z8a4−14z6a4 + 13z4a4−10z2a4 + 3a4 + 3z7a3−8z5a3 + 4z3a3 + z6a2−3z4a2 + 2z2a2 |
| The A2 invariant | Data:K11a295/QuantumInvariant/A2/1,0 |
| The G2 invariant | Data:K11a295/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["K11a295"];
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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 + 14t2−24t + 27−24t−1 + 14t−2−3t−3 |
In[5]:=
| Conway[K][z]
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Out[5]=
| −3z6−4z4 + 5z2 + 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]=
| { 109, -4 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| 1−3q−1 + 7q−2−11q−3 + 15q−4−17q−5 + 18q−6−15q−7 + 11q−8−7q−9 + 3q−10−q−11 |
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]=
| −z2a10−2a10 + 3z4a8 + 8z2a8 + 4a8−2z6a6−7z4a6−8z2a6−4a6−z6a4−z4a4 + 4z2a4 + 3a4 + z4a2 + 2z2a2 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| z5a13−2z3a13 + za13 + 3z6a12−5z4a12 + z2a12 + 5z7a11−8z5a11 + 3z3a11−2za11 + 6z8a10−11z6a10 + 10z4a10−7z2a10 + 2a10 + 5z9a9−8z7a9 + 5z5a9 + 2z3a9−za9 + 2z10a8 + 5z8a8−24z6a8 + 36z4a8−18z2a8 + 4a8 + 10z9a7−29z7a7 + 35z5a7−16z3a7 + 3za7 + 2z10a6 + 4z8a6−25z6a6 + 37z4a6−22z2a6 + 4a6 + 5z9a5−13z7a5 + 13z5a5−9z3a5 + za5 + 5z8a4−14z6a4 + 13z4a4−10z2a4 + 3a4 + 3z7a3−8z5a3 + 4z3a3 + z6a2−3z4a2 + 2z2a2 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {}
Same Jones Polynomial (up to mirroring,
):
{K11a120,}
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["K11a295"];
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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 + 14t2−24t + 27−24t−1 + 14t−2−3t−3, 1−3q−1 + 7q−2−11q−3 + 15q−4−17q−5 + 18q−6−15q−7 + 11q−8−7q−9 + 3q−10−q−11 } |
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]=
| {K11a120,} |
[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 K11a295. 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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