K11a305
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a305's page at Knotilus! Visit K11a305's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X12,4,13,3 X10,5,11,6 X22,8,1,7 X16,9,17,10 X18,12,19,11 X20,13,21,14 X8,15,9,16 X4,18,5,17 X2,19,3,20 X14,21,15,22 |
| Gauss code | 1, -10, 2, -9, 3, -1, 4, -8, 5, -3, 6, -2, 7, -11, 8, -5, 9, -6, 10, -7, 11, -4 |
| Dowker-Thistlethwaite code | 6 12 10 22 16 18 20 8 4 2 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 + 6t3−16t2 + 28t−33 + 28t−1−16t−2 + 6t−3−t−4 |
| Conway polynomial | −z8−2z6 + 2z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 135, -2 } |
| Jones polynomial | −q4 + 4q3−9q2 + 14q−18 + 22q−1−21q−2 + 19q−3−14q−4 + 8q−5−4q−6 + q−7 |
| HOMFLY-PT polynomial (db, data sources) | −a2z8 + a4z6−5a2z6 + 2z6 + 3a4z4−9a2z4−z4a−2 + 7z4 + 2a4z2−5a2z2−2z2a−2 + 7z2−a4 + a2−a−2 + 2 |
| Kauffman polynomial (db, data sources) | 3a2z10 + 3z10 + 10a3z9 + 16az9 + 6z9a−1 + 14a4z8 + 15a2z8 + 4z8a−2 + 5z8 + 12a5z7−14a3z7−44az7−17z7a−1 + z7a−3 + 8a6z6−27a4z6−64a2z6−13z6a−2−42z6 + 4a7z5−15a5z5−5a3z5 + 26az5 + 9z5a−1−3z5a−3 + a8z4−6a6z4 + 20a4z4 + 64a2z4 + 13z4a−2 + 50z4−2a7z3 + 4a5z3 + 9a3z3 + 3az3 + 3z3a−1 + 3z3a−3−6a4z2−19a2z2−6z2a−2−19z2 + a5z−2az−2za−1−za−3−a4−a2 + a−2 + 2 |
| The A2 invariant | q20−2q18 + 2q16−3q14−2q12 + 3q10−3q8 + 6q6−q4 + 2q2 + 2−3q−2 + 3q−4−2q−6 + q−10−q−12 |
| The G2 invariant | Data:K11a305/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["K11a305"];
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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 + 6t3−16t2 + 28t−33 + 28t−1−16t−2 + 6t−3−t−4 |
In[5]:=
| Conway[K][z]
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Out[5]=
| −z8−2z6 + 2z2 + 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]=
| { 135, -2 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| −q4 + 4q3−9q2 + 14q−18 + 22q−1−21q−2 + 19q−3−14q−4 + 8q−5−4q−6 + q−7 |
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]=
| −a2z8 + a4z6−5a2z6 + 2z6 + 3a4z4−9a2z4−z4a−2 + 7z4 + 2a4z2−5a2z2−2z2a−2 + 7z2−a4 + a2−a−2 + 2 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| 3a2z10 + 3z10 + 10a3z9 + 16az9 + 6z9a−1 + 14a4z8 + 15a2z8 + 4z8a−2 + 5z8 + 12a5z7−14a3z7−44az7−17z7a−1 + z7a−3 + 8a6z6−27a4z6−64a2z6−13z6a−2−42z6 + 4a7z5−15a5z5−5a3z5 + 26az5 + 9z5a−1−3z5a−3 + a8z4−6a6z4 + 20a4z4 + 64a2z4 + 13z4a−2 + 50z4−2a7z3 + 4a5z3 + 9a3z3 + 3az3 + 3z3a−1 + 3z3a−3−6a4z2−19a2z2−6z2a−2−19z2 + a5z−2az−2za−1−za−3−a4−a2 + a−2 + 2 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {K11a157, K11a264,}
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["K11a305"];
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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 + 6t3−16t2 + 28t−33 + 28t−1−16t−2 + 6t−3−t−4, −q4 + 4q3−9q2 + 14q−18 + 22q−1−21q−2 + 19q−3−14q−4 + 8q−5−4q−6 + q−7 } |
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]=
| {K11a157, K11a264,} |
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 = -2 is the signature of K11a305. 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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