K11a302
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a302's page at Knotilus! Visit K11a302's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X10,3,11,4 X18,5,19,6 X14,7,15,8 X20,10,21,9 X4,11,5,12 X22,13,1,14 X8,15,9,16 X12,18,13,17 X2,19,3,20 X16,21,17,22 |
| Gauss code | 1, -10, 2, -6, 3, -1, 4, -8, 5, -2, 6, -9, 7, -4, 8, -11, 9, -3, 10, -5, 11, -7 |
| Dowker-Thistlethwaite code | 6 10 18 14 20 4 22 8 12 2 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 | t4−7t3 + 20t2−33t + 39−33t−1 + 20t−2−7t−3 + t−4 |
| Conway polynomial | z8 + z6−2z4 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 161, -4 } |
| Jones polynomial | −q + 5−10q−1 + 17q−2−22q−3 + 26q−4−26q−5 + 22q−6−17q−7 + 10q−8−4q−9 + q−10 |
| HOMFLY-PT polynomial (db, data sources) | z4a8 + 2z2a8 + a8−2z6a6−6z4a6−5z2a6−2a6 + z8a4 + 4z6a4 + 5z4a4 + 2z2a4−z6a2−2z4a2 + z2a2 + 2a2 |
| Kauffman polynomial (db, data sources) | z4a12 + 4z5a11 + 10z6a10−7z4a10 + 3z2a10 + 17z7a9−24z5a9 + 14z3a9−3za9 + 19z8a8−32z6a8 + 17z4a8−5z2a8 + a8 + 13z9a7−12z7a7−18z5a7 + 16z3a7−5za7 + 4z10a6 + 20z8a6−73z6a6 + 59z4a6−18z2a6 + 2a6 + 21z9a5−53z7a5 + 29z5a5−za5 + 4z10a4 + 6z8a4−46z6a4 + 47z4a4−11z2a4 + 8z9a3−23z7a3 + 17z5a3−z3a3 + za3 + 5z8a2−15z6a2 + 13z4a2−z2a2−2a2 + z7a−2z5a + z3a |
| The A2 invariant | q30−q28 + 3q24−4q22 + 3q20−3q18−2q16 + 3q14−5q12 + 6q10−3q8 + 2q6 + 3q4−2q2 + 3−q−2 |
| The G2 invariant | Data:K11a302/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["K11a302"];
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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]=
| t4−7t3 + 20t2−33t + 39−33t−1 + 20t−2−7t−3 + t−4 |
In[5]:=
| Conway[K][z]
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Out[5]=
| z8 + z6−2z4 + 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]=
| { 161, -4 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| −q + 5−10q−1 + 17q−2−22q−3 + 26q−4−26q−5 + 22q−6−17q−7 + 10q−8−4q−9 + q−10 |
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]=
| z4a8 + 2z2a8 + a8−2z6a6−6z4a6−5z2a6−2a6 + z8a4 + 4z6a4 + 5z4a4 + 2z2a4−z6a2−2z4a2 + z2a2 + 2a2 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| z4a12 + 4z5a11 + 10z6a10−7z4a10 + 3z2a10 + 17z7a9−24z5a9 + 14z3a9−3za9 + 19z8a8−32z6a8 + 17z4a8−5z2a8 + a8 + 13z9a7−12z7a7−18z5a7 + 16z3a7−5za7 + 4z10a6 + 20z8a6−73z6a6 + 59z4a6−18z2a6 + 2a6 + 21z9a5−53z7a5 + 29z5a5−za5 + 4z10a4 + 6z8a4−46z6a4 + 47z4a4−11z2a4 + 8z9a3−23z7a3 + 17z5a3−z3a3 + za3 + 5z8a2−15z6a2 + 13z4a2−z2a2−2a2 + z7a−2z5a + z3a |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {}
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["K11a302"];
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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]=
| { t4−7t3 + 20t2−33t + 39−33t−1 + 20t−2−7t−3 + t−4, −q + 5−10q−1 + 17q−2−22q−3 + 26q−4−26q−5 + 22q−6−17q−7 + 10q−8−4q−9 + q−10 } |
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]=
| {} |
[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 K11a302. 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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