K11a223
From Knot Atlas
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![]() (Knotscape image) | See the full Hoste-Thistlethwaite Table of 11 Crossing Knots.
Visit K11a223's page at Knotilus! Visit K11a223's page at the original Knot Atlas! |
[edit] Knot presentations
| Planar diagram presentation | X4251 X12,4,13,3 X18,6,19,5 X20,8,21,7 X16,10,17,9 X2,12,3,11 X22,13,1,14 X8,16,9,15 X10,18,11,17 X6,20,7,19 X14,21,15,22 |
| Gauss code | 1, -6, 2, -1, 3, -10, 4, -8, 5, -9, 6, -2, 7, -11, 8, -5, 9, -3, 10, -4, 11, -7 |
| Dowker-Thistlethwaite code | 4 12 18 20 16 2 22 8 10 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 + 5t3−10t2 + 14t−15 + 14t−1−10t−2 + 5t−3−t−4 |
| Conway polynomial | −z8−3z6 + 3z2 + 1 |
| 2nd Alexander ideal (db, data sources) | {1} |
| Determinant and Signature | { 75, 6 } |
| Jones polynomial | −q12 + 3q11−5q10 + 8q9−11q8 + 11q7−11q6 + 10q5−7q4 + 5q3−2q2 + q |
| HOMFLY-PT polynomial (db, data sources) | −z8a−6 + z6a−4−6z6a−6 + 2z6a−8 + 5z4a−4−13z4a−6 + 9z4a−8−z4a−10 + 8z2a−4−13z2a−6 + 11z2a−8−3z2a−10 + 4a−4−5a−6 + 3a−8−a−10 |
| Kauffman polynomial (db, data sources) | z10a−6 + z10a−8 + 2z9a−5 + 6z9a−7 + 4z9a−9 + z8a−4 + z8a−6 + 8z8a−8 + 8z8a−10−10z7a−5−22z7a−7−3z7a−9 + 9z7a−11−6z6a−4−22z6a−6−44z6a−8−21z6a−10 + 7z6a−12 + 15z5a−5 + 15z5a−7−25z5a−9−20z5a−11 + 5z5a−13 + 13z4a−4 + 43z4a−6 + 55z4a−8 + 14z4a−10−8z4a−12 + 3z4a−14−5z3a−5 + 9z3a−7 + 30z3a−9 + 12z3a−11−3z3a−13 + z3a−15−12z2a−4−27z2a−6−22z2a−8−6z2a−10−z2a−14−3za−5−6za−7−6za−9−3za−11 + 4a−4 + 5a−6 + 3a−8 + a−10 |
| The A2 invariant | q−4 + 2q−8 + q−10 + 2q−14−2q−16 + 2q−18−2q−20−q−22−2q−26 + 2q−28 + q−32−q−36 |
| The G2 invariant | q−22−q−24 + 5q−26−7q−28 + 10q−30−9q−32 + 3q−34 + 15q−36−31q−38 + 47q−40−46q−42 + 27q−44 + 13q−46−57q−48 + 91q−50−90q−52 + 63q−54−4q−56−56q−58 + 93q−60−96q−62 + 63q−64−7q−66−48q−68 + 69q−70−58q−72 + 19q−74 + 30q−76−66q−78 + 71q−80−48q−82−4q−84 + 57q−86−105q−88 + 112q−90−80q−92 + 26q−94 + 44q−96−100q−98 + 121q−100−100q−102 + 47q−104 + 16q−106−71q−108 + 85q−110−57q−112 + 14q−114 + 31q−116−52q−118 + 47q−120−14q−122−29q−124 + 54q−126−61q−128 + 47q−130−10q−132−25q−134 + 48q−136−53q−138 + 47q−140−31q−142 + 8q−144 + 9q−146−27q−148 + 33q−150−32q−152 + 26q−154−13q−156 + 4q−158 + 7q−160−19q−162 + 21q−164−21q−166 + 15q−168−7q−170 + q−172 + 6q−174−11q−176 + 13q−178−10q−180 + 7q−182−2q−184−q−186 + 2q−188−4q−190 + 3q−192−2q−194 + q−196 |
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["K11a223"];
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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 + 5t3−10t2 + 14t−15 + 14t−1−10t−2 + 5t−3−t−4 |
In[5]:=
| Conway[K][z]
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Out[5]=
| −z8−3z6 + 3z2 + 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]=
| { 75, 6 } |
In[8]:=
| Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
| −q12 + 3q11−5q10 + 8q9−11q8 + 11q7−11q6 + 10q5−7q4 + 5q3−2q2 + q |
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−6 + z6a−4−6z6a−6 + 2z6a−8 + 5z4a−4−13z4a−6 + 9z4a−8−z4a−10 + 8z2a−4−13z2a−6 + 11z2a−8−3z2a−10 + 4a−4−5a−6 + 3a−8−a−10 |
In[10]:=
| Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
| z10a−6 + z10a−8 + 2z9a−5 + 6z9a−7 + 4z9a−9 + z8a−4 + z8a−6 + 8z8a−8 + 8z8a−10−10z7a−5−22z7a−7−3z7a−9 + 9z7a−11−6z6a−4−22z6a−6−44z6a−8−21z6a−10 + 7z6a−12 + 15z5a−5 + 15z5a−7−25z5a−9−20z5a−11 + 5z5a−13 + 13z4a−4 + 43z4a−6 + 55z4a−8 + 14z4a−10−8z4a−12 + 3z4a−14−5z3a−5 + 9z3a−7 + 30z3a−9 + 12z3a−11−3z3a−13 + z3a−15−12z2a−4−27z2a−6−22z2a−8−6z2a−10−z2a−14−3za−5−6za−7−6za−9−3za−11 + 4a−4 + 5a−6 + 3a−8 + a−10 |
[edit] "Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {K11n148,}
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["K11a223"];
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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 + 5t3−10t2 + 14t−15 + 14t−1−10t−2 + 5t−3−t−4, −q12 + 3q11−5q10 + 8q9−11q8 + 11q7−11q6 + 10q5−7q4 + 5q3−2q2 + q } |
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]=
| {K11n148,} |
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 = 6 is the signature of K11a223. 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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