K11a293
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a293's page at Knotilus! Visit K11a293's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X10,4,11,3 X16,5,17,6 X22,8,1,7 X4,10,5,9 X18,11,19,12 X20,13,21,14 X8,15,9,16 X2,17,3,18 X12,19,13,20 X14,21,15,22 |
| Gauss code | 1, -9, 2, -5, 3, -1, 4, -8, 5, -2, 6, -10, 7, -11, 8, -3, 9, -6, 10, -7, 11, -4 |
| Dowker-Thistlethwaite code | 6 10 16 22 4 18 20 8 2 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 | t4−5t3 + 12t2−15t + 15−15t−1 + 12t−2−5t−3 + t−4 |
| Conway polynomial | z8 + 3z6 + 2z4 + 4z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {3,t + 1} |
| Determinant and Signature | { 81, -4 } |
| Jones polynomial | q2−3q + 5−8q−1 + 11q−2−11q−3 + 13q−4−11q−5 + 8q−6−6q−7 + 3q−8−q−9 |
| HOMFLY-PT polynomial (db, data sources) | a4z8−a6z6 + 6a4z6−2a2z6−4a6z4 + 14a4z4−9a2z4 + z4−5a6z2 + 17a4z2−11a2z2 + 3z2−4a6 + 8a4−4a2 + 1 |
| Kauffman polynomial (db, data sources) | z3a11 + 3z4a10 + 6z5a9−5z3a9 + 2za9 + 8z6a8−10z4a8 + 2z2a8 + 9z7a7−16z5a7 + 4z3a7−2za7 + 9z8a6−24z6a6 + 18z4a6−11z2a6 + 4a6 + 6z9a5−15z7a5 + z5a5 + 10z3a5−6za5 + 2z10a4 + 3z8a4−36z6a4 + 51z4a4−25z2a4 + 8a4 + 9z9a3−40z7a3 + 50z5a3−15z3a3−2za3 + 2z10a2−5z8a2−9z6a2 + 28z4a2−17z2a2 + 4a2 + 3z9a−16z7a + 27z5a−15z3a + z8−5z6 + 8z4−5z2 + 1 |
| The A2 invariant | −q26 + q24−2q22−q20−q18−q16 + 4q14 + 4q10 + q8 + q4−2q2−q−2 + q−6 |
| The G2 invariant | Data:K11a293/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["K11a293"];
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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 + 12t2−15t + 15−15t−1 + 12t−2−5t−3 + t−4 |
In[5]:=
| Conway[K][z]
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Out[5]=
| z8 + 3z6 + 2z4 + 4z2 + 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]=
| {3,t + 1} |
In[7]:=
| {KnotDet[K], KnotSignature[K]}
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Out[7]=
| { 81, -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 + 5−8q−1 + 11q−2−11q−3 + 13q−4−11q−5 + 8q−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 + 17a4z2−11a2z2 + 3z2−4a6 + 8a4−4a2 + 1 |
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 + 6z5a9−5z3a9 + 2za9 + 8z6a8−10z4a8 + 2z2a8 + 9z7a7−16z5a7 + 4z3a7−2za7 + 9z8a6−24z6a6 + 18z4a6−11z2a6 + 4a6 + 6z9a5−15z7a5 + z5a5 + 10z3a5−6za5 + 2z10a4 + 3z8a4−36z6a4 + 51z4a4−25z2a4 + 8a4 + 9z9a3−40z7a3 + 50z5a3−15z3a3−2za3 + 2z10a2−5z8a2−9z6a2 + 28z4a2−17z2a2 + 4a2 + 3z9a−16z7a + 27z5a−15z3a + z8−5z6 + 8z4−5z2 + 1 |
[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["K11a293"];
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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 + 12t2−15t + 15−15t−1 + 12t−2−5t−3 + t−4, q2−3q + 5−8q−1 + 11q−2−11q−3 + 13q−4−11q−5 + 8q−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]=
| {} |
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 K11a293. 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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