K11a327
From Knot Atlas
|
|
|
|
 (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a327's page at Knotilus! Visit K11a327's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X12,4,13,3 X18,6,19,5 X16,7,17,8 X14,10,15,9 X4,12,5,11 X20,14,21,13 X22,15,1,16 X2,18,3,17 X10,20,11,19 X8,21,9,22 |
| Gauss code | 1, -9, 2, -6, 3, -1, 4, -11, 5, -10, 6, -2, 7, -5, 8, -4, 9, -3, 10, -7, 11, -8 |
| Dowker-Thistlethwaite code | 6 12 18 16 14 4 20 22 2 10 8 |
| A Braid Representative |
| ||||||
| A Morse Link Presentation | 
|
[edit] Three dimensional invariants
|
[edit] Four dimensional invariants
|
[edit] Polynomial invariants
| Alexander polynomial | 3t3−17t2 + 44t−59 + 44t−1−17t−2 + 3t−3 |
| Conway polynomial | 3z6 + z4 + 3z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 187, 2 } |
| Jones polynomial | q9−5q8 + 11q7−19q6 + 26q5−30q4 + 31q3−26q2 + 20q−12 + 5q−1−q−2 |
| HOMFLY-PT polynomial (db, data sources) | z6a−2 + 2z6a−4 + 5z4a−4−3z4a−6−z4−z2a−2 + 7z2a−4−4z2a−6 + z2a−8 + 3a−4−2a−6 |
| Kauffman polynomial (db, data sources) | 4z10a−4 + 4z10a−6 + 13z9a−3 + 23z9a−5 + 10z9a−7 + 17z8a−2 + 26z8a−4 + 19z8a−6 + 10z8a−8 + 12z7a−1−8z7a−3−36z7a−5−11z7a−7 + 5z7a−9−26z6a−2−71z6a−4−61z6a−6−20z6a−8 + z6a−10 + 5z6 + az5−14z5a−1−16z5a−3−3z5a−5−11z5a−7−9z5a−9 + 14z4a−2 + 54z4a−4 + 50z4a−6 + 12z4a−8−z4a−10−3z4 + 4z3a−1 + 15z3a−3 + 23z3a−5 + 16z3a−7 + 4z3a−9−4z2a−2−16z2a−4−15z2a−6−3z2a−8−za−1−4za−3−8za−5−5za−7 + 3a−4 + 2a−6 |
| The A2 invariant | Data:K11a327/QuantumInvariant/A2/1,0 |
| The G2 invariant | Data:K11a327/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[$Path, "C:/drorbn/projects/KAtlas/"];
<< KnotTheory`
|
Loading KnotTheory` version of August 31, 2006, 11:25:27.5625.
|
In[3]:=
| K = Knot["K11a327"];
|
In[4]:=
| Alexander[K][t]
|
KnotTheory::loading: Loading precomputed data in PD4Knots`.
|
Out[4]=
| 3t3−17t2 + 44t−59 + 44t−1−17t−2 + 3t−3 |
In[5]:=
| Conway[K][z]
|
Out[5]=
| 3z6 + z4 + 3z2 + 1 |
In[6]:=
| Alexander[K, 2][t]
|
KnotTheory::credits: The program Alexander[K, r] to compute Alexander ideals was written by Jana Archibald at the University of Toronto in the summer of 2005.
|
Out[6]=
| {1} |
In[7]:=
| {KnotDet[K], KnotSignature[K]}
|
Out[7]=
| { 187, 2 } |
In[8]:=
| Jones[K][q]
|
KnotTheory::loading: Loading precomputed data in Jones4Knots`.
|
Out[8]=
| q9−5q8 + 11q7−19q6 + 26q5−30q4 + 31q3−26q2 + 20q−12 + 5q−1−q−2 |
In[9]:=
| HOMFLYPT[K][a, z]
|
KnotTheory::credits: The HOMFLYPT program was written by Scott Morrison.
|
Out[9]=
| z6a−2 + 2z6a−4 + 5z4a−4−3z4a−6−z4−z2a−2 + 7z2a−4−4z2a−6 + z2a−8 + 3a−4−2a−6 |
In[10]:=
| Kauffman[K][a, z]
|
KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
|
Out[10]=
| 4z10a−4 + 4z10a−6 + 13z9a−3 + 23z9a−5 + 10z9a−7 + 17z8a−2 + 26z8a−4 + 19z8a−6 + 10z8a−8 + 12z7a−1−8z7a−3−36z7a−5−11z7a−7 + 5z7a−9−26z6a−2−71z6a−4−61z6a−6−20z6a−8 + z6a−10 + 5z6 + az5−14z5a−1−16z5a−3−3z5a−5−11z5a−7−9z5a−9 + 14z4a−2 + 54z4a−4 + 50z4a−6 + 12z4a−8−z4a−10−3z4 + 4z3a−1 + 15z3a−3 + 23z3a−5 + 16z3a−7 + 4z3a−9−4z2a−2−16z2a−4−15z2a−6−3z2a−8−za−1−4za−3−8za−5−5za−7 + 3a−4 + 2a−6 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {}
Same Jones Polynomial (up to mirroring, 
):
{}
Computer Talk
The above data is available with the Mathematica package
KnotTheory`. Your input (in red) is realistic; all else should have the same content as in a real mathematica session, but with different formatting.
(The path below may be different on your system, and possibly also the KnotTheory` date)
In[1]:=
| AppendTo[$Path, "C:/drorbn/projects/KAtlas/"];
<< KnotTheory`
|
Loading KnotTheory` version of May 31, 2006, 14:15:20.091.
|
In[3]:=
| K = Knot["K11a327"];
|
In[4]:=
| {A = Alexander[K][t], J = Jones[K][q]}
|
KnotTheory::loading: Loading precomputed data in PD4Knots`.
|
KnotTheory::loading: Loading precomputed data in Jones4Knots`.
|
Out[4]=
| { 3t3−17t2 + 44t−59 + 44t−1−17t−2 + 3t−3, q9−5q8 + 11q7−19q6 + 26q5−30q4 + 31q3−26q2 + 20q−12 + 5q−1−q−2 } |
In[5]:=
| DeleteCases[Select[AllKnots[], (A === Alexander[#][t]) &], K]
|
KnotTheory::loading: Loading precomputed data in DTCode4KnotsTo11`.
|
KnotTheory::credits: The GaussCode to PD conversion was written by Siddarth Sankaran at the University of Toronto in the summer of 2005.
|
Out[5]=
| {} |
In[6]:=
| DeleteCases[
Select[
AllKnots[],
(J === Jones[#][q] || (J /. q -> 1/q) === Jones[#][q]) &
],
K
]
|
KnotTheory::loading: Loading precomputed data in Jones4Knots11`.
|
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 K11a327. Nonzero entries off the critical diagonals (if any exist) are highlighted in red. |
|
| Integral Khovanov Homology
(db, data source) |
|
[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. |
|
