K11a301
From Knot Atlas
|
|
|
|
![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a301's page at Knotilus! Visit K11a301's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X6271 X10,3,11,4 X18,5,19,6 X14,7,15,8 X16,10,17,9 X4,11,5,12 X22,13,1,14 X20,16,21,15 X12,18,13,17 X2,19,3,20 X8,21,9,22 |
| Gauss code | 1, -10, 2, -6, 3, -1, 4, -11, 5, -2, 6, -9, 7, -4, 8, -5, 9, -3, 10, -8, 11, -7 |
| Dowker-Thistlethwaite code | 6 10 18 14 16 4 22 20 12 2 8 |
| A Braid Representative | | ||||
| A Morse Link Presentation |
|
[edit] Three dimensional invariants
|
[edit] Four dimensional invariants
|
[edit] Polynomial invariants
| Alexander polynomial | −t4 + 7t3−22t2 + 43t−53 + 43t−1−22t−2 + 7t−3−t−4 |
| Conway polynomial | −z8−z6 + 2z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 199, -2 } |
| Jones polynomial | q3−5q2 + 12q−20 + 28q−1−32q−2 + 33q−3−28q−4 + 21q−5−13q−6 + 5q−7−q−8 |
| HOMFLY-PT polynomial (db, data sources) | −a2z8 + 2a4z6−4a2z6 + z6−a6z4 + 5a4z4−6a2z4 + 2z4−a6z2 + 4a4z2−2a2z2 + z2−a6 + a4 + a2 |
| Kauffman polynomial (db, data sources) | 5a4z10 + 5a2z10 + 15a5z9 + 27a3z9 + 12az9 + 19a6z8 + 26a4z8 + 18a2z8 + 11z8 + 13a7z7−11a5z7−47a3z7−18az7 + 5z7a−1 + 5a8z6−29a6z6−70a4z6−59a2z6 + z6a−2−22z6 + a9z5−15a7z5−13a5z5 + 13a3z5 + 2az5−8z5a−1−2a8z4 + 16a6z4 + 46a4z4 + 43a2z4−z4a−2 + 14z4 + 6a7z3 + 10a5z3 + 5a3z3 + 4az3 + 3z3a−1−5a6z2−10a4z2−8a2z2−3z2−2a7z−2a5z + a6 + a4−a2 |
| The A2 invariant | −q24 + 2q22−q20−4q18 + 5q16−5q14 + 3q12 + 2q10−3q8 + 7q6−6q4 + 6q2−1−3q−2 + 4q−4−3q−6 + q−8 |
| The G2 invariant | Data:K11a301/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[$Path, "C:/drorbn/projects/KAtlas/"];
<< KnotTheory`
|
Loading KnotTheory` version of August 31, 2006, 11:25:27.5625.
|
In[3]:=
| K = Knot["K11a301"];
|
In[4]:=
| Alexander[K][t]
|
KnotTheory::loading: Loading precomputed data in PD4Knots`.
|
Out[4]=
| −t4 + 7t3−22t2 + 43t−53 + 43t−1−22t−2 + 7t−3−t−4 |
In[5]:=
| Conway[K][z]
|
Out[5]=
| −z8−z6 + 2z2 + 1 |
In[6]:=
| Alexander[K, 2][t]
|
KnotTheory::credits: The program Alexander[K, r] to compute Alexander ideals was written by Jana Archibald at the University of Toronto in the summer of 2005.
|
Out[6]=
| {1} |
In[7]:=
| {KnotDet[K], KnotSignature[K]}
|
Out[7]=
| { 199, -2 } |
In[8]:=
| Jones[K][q]
|
KnotTheory::loading: Loading precomputed data in Jones4Knots`.
|
Out[8]=
| q3−5q2 + 12q−20 + 28q−1−32q−2 + 33q−3−28q−4 + 21q−5−13q−6 + 5q−7−q−8 |
In[9]:=
| HOMFLYPT[K][a, z]
|
KnotTheory::credits: The HOMFLYPT program was written by Scott Morrison.
|
Out[9]=
| −a2z8 + 2a4z6−4a2z6 + z6−a6z4 + 5a4z4−6a2z4 + 2z4−a6z2 + 4a4z2−2a2z2 + z2−a6 + a4 + a2 |
In[10]:=
| Kauffman[K][a, z]
|
KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
|
Out[10]=
| 5a4z10 + 5a2z10 + 15a5z9 + 27a3z9 + 12az9 + 19a6z8 + 26a4z8 + 18a2z8 + 11z8 + 13a7z7−11a5z7−47a3z7−18az7 + 5z7a−1 + 5a8z6−29a6z6−70a4z6−59a2z6 + z6a−2−22z6 + a9z5−15a7z5−13a5z5 + 13a3z5 + 2az5−8z5a−1−2a8z4 + 16a6z4 + 46a4z4 + 43a2z4−z4a−2 + 14z4 + 6a7z3 + 10a5z3 + 5a3z3 + 4az3 + 3z3a−1−5a6z2−10a4z2−8a2z2−3z2−2a7z−2a5z + a6 + a4−a2 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {}
Same Jones Polynomial (up to mirroring,
):
{}
Computer Talk
The above data is available with the Mathematica package
KnotTheory`. Your input (in red) is realistic; all else should have the same content as in a real mathematica session, but with different formatting.
(The path below may be different on your system, and possibly also the KnotTheory` date)
In[1]:=
| AppendTo[$Path, "C:/drorbn/projects/KAtlas/"];
<< KnotTheory`
|
Loading KnotTheory` version of May 31, 2006, 14:15:20.091.
|
In[3]:=
| K = Knot["K11a301"];
|
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]=
| { −t4 + 7t3−22t2 + 43t−53 + 43t−1−22t−2 + 7t−3−t−4, q3−5q2 + 12q−20 + 28q−1−32q−2 + 33q−3−28q−4 + 21q−5−13q−6 + 5q−7−q−8 } |
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 K11a301. 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. |
|


