K11a315
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a315's page at Knotilus! Visit K11a315's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X12,4,13,3 X16,5,17,6 X18,8,19,7 X22,10,1,9 X4,12,5,11 X20,13,21,14 X10,15,11,16 X2,17,3,18 X8,20,9,19 X14,21,15,22 |
| Gauss code | 1, -9, 2, -6, 3, -1, 4, -10, 5, -8, 6, -2, 7, -11, 8, -3, 9, -4, 10, -7, 11, -5 |
| Dowker-Thistlethwaite code | 6 12 16 18 22 4 20 10 2 8 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 | t4−6t3 + 18t2−33t + 41−33t−1 + 18t−2−6t−3 + t−4 |
| Conway polynomial | z8 + 2z6 + 2z4 + z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 157, 0 } |
| Jones polynomial | q6−4q5 + 9q4−16q3 + 22q2−25q + 26−22q−1 + 17q−2−10q−3 + 4q−4−q−5 |
| HOMFLY-PT polynomial (db, data sources) | z8−a2z6−2z6a−2 + 5z6−3a2z4−7z4a−2 + z4a−4 + 11z4−4a2z2−9z2a−2 + 2z2a−4 + 12z2−2a2−4a−2 + a−4 + 6 |
| Kauffman polynomial (db, data sources) | 3z10a−2 + 3z10 + 10az9 + 17z9a−1 + 7z9a−3 + 13a2z8 + 12z8a−2 + 7z8a−4 + 18z8 + 9a3z7−11az7−32z7a−1−8z7a−3 + 4z7a−5 + 4a4z6−25a2z6−41z6a−2−14z6a−4 + z6a−6−55z6 + a5z5−13a3z5−2az5 + 15z5a−1−6z5a−3−9z5a−5−4a4z4 + 23a2z4 + 39z4a−2 + 8z4a−4−2z4a−6 + 56z4−a5z3 + 7a3z3 + 9az3 + 3z3a−1 + 8z3a−3 + 6z3a−5−11a2z2−19z2a−2−3z2a−4 + z2a−6−26z2−2a3z−4az−4za−1−3za−3−za−5 + 2a2 + 4a−2 + a−4 + 6 |
| The A2 invariant | −q14 + 2q12−4q10 + 2q8 + q6−3q4 + 7q2−3 + 5q−2−q−4−2q−6 + 3q−8−5q−10 + 2q−12−q−16 + q−18 |
| The G2 invariant | Data:K11a315/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["K11a315"];
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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]=
| t4−6t3 + 18t2−33t + 41−33t−1 + 18t−2−6t−3 + t−4 |
In[5]:=
| Conway[K][z]
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Out[5]=
| z8 + 2z6 + 2z4 + z2 + 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]=
| { 157, 0 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| q6−4q5 + 9q4−16q3 + 22q2−25q + 26−22q−1 + 17q−2−10q−3 + 4q−4−q−5 |
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]=
| z8−a2z6−2z6a−2 + 5z6−3a2z4−7z4a−2 + z4a−4 + 11z4−4a2z2−9z2a−2 + 2z2a−4 + 12z2−2a2−4a−2 + a−4 + 6 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| 3z10a−2 + 3z10 + 10az9 + 17z9a−1 + 7z9a−3 + 13a2z8 + 12z8a−2 + 7z8a−4 + 18z8 + 9a3z7−11az7−32z7a−1−8z7a−3 + 4z7a−5 + 4a4z6−25a2z6−41z6a−2−14z6a−4 + z6a−6−55z6 + a5z5−13a3z5−2az5 + 15z5a−1−6z5a−3−9z5a−5−4a4z4 + 23a2z4 + 39z4a−2 + 8z4a−4−2z4a−6 + 56z4−a5z3 + 7a3z3 + 9az3 + 3z3a−1 + 8z3a−3 + 6z3a−5−11a2z2−19z2a−2−3z2a−4 + z2a−6−26z2−2a3z−4az−4za−1−3za−3−za−5 + 2a2 + 4a−2 + a−4 + 6 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {K11a24, K11a26,}
Same Jones Polynomial (up to mirroring,
):
{K11a24, K11a26,}
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["K11a315"];
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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]=
| { t4−6t3 + 18t2−33t + 41−33t−1 + 18t−2−6t−3 + t−4, q6−4q5 + 9q4−16q3 + 22q2−25q + 26−22q−1 + 17q−2−10q−3 + 4q−4−q−5 } |
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]=
| {K11a24, K11a26,} |
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]=
| {K11a24, K11a26,} |
[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 = 0 is the signature of K11a315. 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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