K11a253
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a253's page at Knotilus! Visit K11a253's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X8493 X12,5,13,6 X2837 X18,9,19,10 X20,12,21,11 X4,13,5,14 X10,15,11,16 X22,17,1,18 X14,20,15,19 X16,21,17,22 |
| Gauss code | 1, -4, 2, -7, 3, -1, 4, -2, 5, -8, 6, -3, 7, -10, 8, -11, 9, -5, 10, -6, 11, -9 |
| Dowker-Thistlethwaite code | 6 8 12 2 18 20 4 10 22 14 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 | t4−6t3 + 16t2−27t + 33−27t−1 + 16t−2−6t−3 + t−4 |
| Conway polynomial | z8 + 2z6−z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 133, 0 } |
| Jones polynomial | −q5 + 4q4−9q3 + 15q2−19q + 22−21q−1 + 18q−2−13q−3 + 7q−4−3q−5 + q−6 |
| HOMFLY-PT polynomial (db, data sources) | z8−2a2z6−z6a−2 + 5z6 + a4z4−8a2z4−3z4a−2 + 10z4 + 3a4z2−11a2z2−3z2a−2 + 10z2 + 2a4−5a2−a−2 + 5 |
| Kauffman polynomial (db, data sources) | 2a2z10 + 2z10 + 5a3z9 + 12az9 + 7z9a−1 + 5a4z8 + 9a2z8 + 10z8a−2 + 14z8 + 3a5z7−8a3z7−24az7−5z7a−1 + 8z7a−3 + a6z6−12a4z6−34a2z6−17z6a−2 + 4z6a−4−42z6−8a5z5 + a3z5 + 16az5−6z5a−1−12z5a−3 + z5a−5−3a6z4 + 10a4z4 + 42a2z4 + 12z4a−2−5z4a−4 + 46z4 + 6a5z3 + 4a3z3−az3 + 7z3a−1 + 5z3a−3−z3a−5 + 2a6z2−6a4z2−24a2z2−6z2a−2 + z2a−4−23z2−2a5z−3a3z−2az−2za−1−za−3 + 2a4 + 5a2 + a−2 + 5 |
| The A2 invariant | q18 + 2q12−4q10 + 2q8−2q6−2q4 + 4q2−3 + 6q−2−2q−4 + q−6 + 2q−8−3q−10 + 2q−12−q−14 |
| The G2 invariant | Data:K11a253/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["K11a253"];
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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 + 16t2−27t + 33−27t−1 + 16t−2−6t−3 + t−4 |
In[5]:=
| Conway[K][z]
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Out[5]=
| z8 + 2z6−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]=
| { 133, 0 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| −q5 + 4q4−9q3 + 15q2−19q + 22−21q−1 + 18q−2−13q−3 + 7q−4−3q−5 + q−6 |
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]=
| z8−2a2z6−z6a−2 + 5z6 + a4z4−8a2z4−3z4a−2 + 10z4 + 3a4z2−11a2z2−3z2a−2 + 10z2 + 2a4−5a2−a−2 + 5 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| 2a2z10 + 2z10 + 5a3z9 + 12az9 + 7z9a−1 + 5a4z8 + 9a2z8 + 10z8a−2 + 14z8 + 3a5z7−8a3z7−24az7−5z7a−1 + 8z7a−3 + a6z6−12a4z6−34a2z6−17z6a−2 + 4z6a−4−42z6−8a5z5 + a3z5 + 16az5−6z5a−1−12z5a−3 + z5a−5−3a6z4 + 10a4z4 + 42a2z4 + 12z4a−2−5z4a−4 + 46z4 + 6a5z3 + 4a3z3−az3 + 7z3a−1 + 5z3a−3−z3a−5 + 2a6z2−6a4z2−24a2z2−6z2a−2 + z2a−4−23z2−2a5z−3a3z−2az−2za−1−za−3 + 2a4 + 5a2 + a−2 + 5 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {K11a251,}
Same Jones Polynomial (up to mirroring,
):
{K11a228, K11a251,}
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["K11a253"];
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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 + 16t2−27t + 33−27t−1 + 16t−2−6t−3 + t−4, −q5 + 4q4−9q3 + 15q2−19q + 22−21q−1 + 18q−2−13q−3 + 7q−4−3q−5 + q−6 } |
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]=
| {K11a251,} |
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]=
| {K11a228, K11a251,} |
[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 K11a253. 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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