K11a147
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a147's page at Knotilus! Visit K11a147's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X4251 X10,4,11,3 X16,6,17,5 X20,8,21,7 X2,10,3,9 X22,11,1,12 X18,13,19,14 X8,16,9,15 X12,17,13,18 X6,20,7,19 X14,21,15,22 |
| Gauss code | 1, -5, 2, -1, 3, -10, 4, -8, 5, -2, 6, -9, 7, -11, 8, -3, 9, -7, 10, -4, 11, -6 |
| Dowker-Thistlethwaite code | 4 10 16 20 2 22 18 8 12 6 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 + 6t3−17t2 + 32t−39 + 32t−1−17t−2 + 6t−3−t−4 |
| Conway polynomial | −z8−2z6−z4 + 2z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 151, 2 } |
| Jones polynomial | −q8 + 4q7−10q6 + 16q5−21q4 + 25q3−24q2 + 21q−15 + 9q−1−4q−2 + q−3 |
| HOMFLY-PT polynomial (db, data sources) | −z8a−2−5z6a−2 + 2z6a−4 + z6−10z4a−2 + 7z4a−4−z4a−6 + 3z4−8z2a−2 + 9z2a−4−2z2a−6 + 3z2−2a−2 + 4a−4−2a−6 + 1 |
| Kauffman polynomial (db, data sources) | 2z10a−2 + 2z10a−4 + 6z9a−1 + 13z9a−3 + 7z9a−5 + 15z8a−2 + 19z8a−4 + 11z8a−6 + 7z8 + 4az7−4z7a−1−13z7a−3 + 4z7a−5 + 9z7a−7 + a2z6−41z6a−2−45z6a−4−16z6a−6 + 4z6a−8−15z6−9az5−12z5a−1−15z5a−3−27z5a−5−14z5a−7 + z5a−9−2a2z4 + 32z4a−2 + 34z4a−4 + 10z4a−6−4z4a−8 + 10z4 + 6az3 + 12z3a−1 + 19z3a−3 + 24z3a−5 + 10z3a−7−z3a−9 + a2z2−12z2a−2−14z2a−4−5z2a−6 + z2a−8−3z2−az−3za−1−5za−3−7za−5−4za−7 + 2a−2 + 4a−4 + 2a−6 + 1 |
| The A2 invariant | q8−2q6 + 3q4−2q2−1 + 4q−2−5q−4 + 5q−6−2q−8 + 2q−10 + 3q−12−3q−14 + 4q−16−3q−18−q−20 + q−22−q−24 |
| The G2 invariant | q46−3q44 + 8q42−16q40 + 22q38−25q36 + 14q34 + 18q32−66q30 + 128q28−176q26 + 175q24−101q22−63q20 + 289q18−494q16 + 595q14−503q12 + 187q10 + 276q8−746q6 + 1033q4−982q2 + 583 + 52q−2−689q−4 + 1072q−6−1041q−8 + 605q−10 + 49q−12−639q−14 + 889q−16−697q−18 + 143q−20 + 532q−22−1009q−24 + 1072q−26−654q−28−117q−30 + 932q−32−1485q−34 + 1542q−36−1054q−38 + 200q−40 + 732q−42−1392q−44 + 1563q−46−1188q−48 + 435q−50 + 387q−52−955q−54 + 1059q−56−686q−58 + 53q−60 + 563q−62−860q−64 + 723q−66−231q−68−416q−70 + 919q−72−1075q−74 + 828q−76−285q−78−335q−80 + 801q−82−973q−84 + 831q−86−473q−88 + 42q−90 + 307q−92−501q−94 + 504q−96−370q−98 + 187q−100−9q−102−105q−104 + 149q−106−143q−108 + 99q−110−49q−112 + 12q−114 + 12q−116−19q−118 + 17q−120−13q−122 + 7q−124−3q−126 + q−128 |
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["K11a147"];
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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 + 6t3−17t2 + 32t−39 + 32t−1−17t−2 + 6t−3−t−4 |
In[5]:=
| Conway[K][z]
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Out[5]=
| −z8−2z6−z4 + 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]=
| { 151, 2 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| −q8 + 4q7−10q6 + 16q5−21q4 + 25q3−24q2 + 21q−15 + 9q−1−4q−2 + q−3 |
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]=
| −z8a−2−5z6a−2 + 2z6a−4 + z6−10z4a−2 + 7z4a−4−z4a−6 + 3z4−8z2a−2 + 9z2a−4−2z2a−6 + 3z2−2a−2 + 4a−4−2a−6 + 1 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| 2z10a−2 + 2z10a−4 + 6z9a−1 + 13z9a−3 + 7z9a−5 + 15z8a−2 + 19z8a−4 + 11z8a−6 + 7z8 + 4az7−4z7a−1−13z7a−3 + 4z7a−5 + 9z7a−7 + a2z6−41z6a−2−45z6a−4−16z6a−6 + 4z6a−8−15z6−9az5−12z5a−1−15z5a−3−27z5a−5−14z5a−7 + z5a−9−2a2z4 + 32z4a−2 + 34z4a−4 + 10z4a−6−4z4a−8 + 10z4 + 6az3 + 12z3a−1 + 19z3a−3 + 24z3a−5 + 10z3a−7−z3a−9 + a2z2−12z2a−2−14z2a−4−5z2a−6 + z2a−8−3z2−az−3za−1−5za−3−7za−5−4za−7 + 2a−2 + 4a−4 + 2a−6 + 1 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {}
Same Jones Polynomial (up to mirroring,
):
{K11a322,}
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["K11a147"];
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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 + 6t3−17t2 + 32t−39 + 32t−1−17t−2 + 6t−3−t−4, −q8 + 4q7−10q6 + 16q5−21q4 + 25q3−24q2 + 21q−15 + 9q−1−4q−2 + q−3 } |
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]=
| {} |
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]=
| {K11a322,} |
[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 K11a147. 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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