Rolfsen Splice Base: Difference between revisions
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<*InOut[1]; KnotTheoryWelcomeMessage[]*> |
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<td><pre style="color: blue; border: 0px; padding: 0em">In[1]:= </pre></td> |
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<td align=left><pre style="color: red; border: 0px; padding: 0em"><< KnotTheory`</pre></td> |
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<tr valign=top><td colspan=2><pre style="border: 0px; padding: 0em"><*InOut[1]; KnotTheoryWelcomeMessage[]*></pre></td></tr> |
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<*InOut["PD[``]", K]*> |
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<*InOut["GaussCode[``]", K]*> |
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<*InOut["DTCode[``]", K]*> |
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<*InOut["br = BR[``]", K]*> |
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<*InOut["{First[br], Crossings[br]}"]*> |
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<*InOut["BraidIndex[``]", K]*> |
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<*GraphicsBox["`1`_`2`_ML.gif", "Show[DrawMorseLink[Knot[`1`, `2`]]]", n, k]*> |
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"(#[``]&) /@ {SymmetryType, UnknottingNumber, ThreeGenus, BridgeIndex, SuperBridgeIndex, NakanishiIndex}", K |
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<*InOut["alex = Alexander[``][t]", K]*> |
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<*InOut["Conway[``][z]", K]*> |
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<*InOut["Select[AllKnots[], (alex === Alexander[#][t])&]"]*> |
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<*InOut["{KnotDet[`1`], KnotSignature[`1`]}", K]*> |
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<*InOut["Jones[``][q]", K]*> |
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"Select[AllKnots[], (J === Jones[#][q] || (J /. q-> 1/q) === Jones[#][q])&]" |
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<*InOut["A2Invariant[``][q]", K]*> |
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<*InOut["HOMFLYPT[``][a, z]", K]*> |
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<*InOut["Kauffman[``][a, z]", K]*> |
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<*InOut["{Vassiliev[2][`1`], Vassiliev[3][`1`]}", K]*> |
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<*InOut["Kh[``][q, t]", K]*> |
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<* If[ColouredJones[K, 2] === NotAvailable, "", |
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] *> |
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{| width=100% |
{| width=100% |
Revision as of 21:59, 29 August 2005
- REDIRECT Template:Splice Base Notice
[[Image:Data:Rolfsen Splice Base/Previous Knot.gif|80px|link=Data:Rolfsen Splice Base/Previous Knot]] |
[[Image:Data:Rolfsen Splice Base/Next Knot.gif|80px|link=Data:Rolfsen Splice Base/Next Knot]] |
File:Rolfsen Splice Base.gif | Visit <*n*>&id=<*k*> Rolfsen Splice Base's page at the Knot Server (KnotPlot driven, includes 3D interactive images!)
Visit [<*KnotilusURL[K]*> Rolfsen Splice Base's page] at Knotilus! Visit <*n*>.<*k*>.html Rolfsen Splice Base's page at the original Knot Atlas! |
Rolfsen Splice Base Further Notes and Views
Knot presentations
Minimum Braid Representative: {{{braid_table}}} Length is {{{braid_crossings}}}, width is {{{braid_width}}}. Braid index is {{{braid_index}}}. |
Three dimensional invariants
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[edit Notes for Rolfsen Splice Base's three dimensional invariants] |
Four dimensional invariants
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[edit Notes for Rolfsen Splice Base's four dimensional invariants] |
Polynomial invariants
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]:=
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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]:=
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K = Knot["Rolfsen Splice Base"];
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In[4]:=
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Alexander[K][t]
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KnotTheory::loading: Loading precomputed data in PD4Knots`.
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Out[4]=
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Data:Rolfsen Splice Base/Alexander Polynomial |
In[5]:=
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Conway[K][z]
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Out[5]=
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Data:Rolfsen Splice Base/Conway Polynomial |
In[6]:=
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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]=
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Data:Rolfsen Splice Base/2nd AlexanderIdeal |
In[7]:=
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{KnotDet[K], KnotSignature[K]}
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Out[7]=
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{ Data:Rolfsen Splice Base/Determinant, Data:Rolfsen Splice Base/Signature } |
In[8]:=
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Jones[K][q]
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
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Data:Rolfsen Splice Base/Jones Polynomial |
In[9]:=
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HOMFLYPT[K][a, z]
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KnotTheory::credits: The HOMFLYPT program was written by Scott Morrison.
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Out[9]=
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Data:Rolfsen Splice Base/HOMFLYPT Polynomial |
In[10]:=
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Kauffman[K][a, z]
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KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.
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Out[10]=
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Data:Rolfsen Splice Base/Kauffman Polynomial |
"Similar" Knots (within the Atlas)
Same Alexander/Conway Polynomial: {<* alex = Alexander[K][t];
others = DeleteCases[Select[AllKnots[], (alex === Alexander[#][t])&], K]; If[others === {}, "", StringJoin[("[["<>NameString[#]<>"]], ")& /@ others]] *>}
Same Jones Polynomial (up to mirroring, ): {<* J = Jones[Knot[n,k]][q];
others = DeleteCases[Select[AllKnots[], (J === Jones[#][q]}
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]:=
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K = Knot["Rolfsen Splice Base"];
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In[4]:=
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{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]=
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{ Data:Rolfsen Splice Base/Alexander Polynomial, Data:Rolfsen Splice Base/Jones Polynomial } |
In[5]:=
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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]=
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{<* alex = Alexander[K][t];
others = DeleteCases[Select[AllKnots[], (alex === Alexander[#][t])&], K]; If[others === {}, "", StringJoin[("[["<>NameString[#]<>"]], ")& /@ others]] *>} |
In[6]:=
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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]=
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{<* J = Jones[Knot[n,k]][q];
others = DeleteCases[Select[AllKnots[], (J === Jones[#][q]} |
Vassiliev invariants
V2 and V3: | (Data:Rolfsen Splice Base/V 2, Data:Rolfsen Splice Base/V 3) |
V2,1 through V6,9 were provided by Petr Dunin-Barkowski <barkovs@itep.ru>, Andrey Smirnov <asmirnov@itep.ru>, and Alexei Sleptsov <sleptsov@itep.ru> and uploaded on October 2010 by User:Drorbn. Note that they are normalized differently than V2 and V3.
Khovanov Homology
The coefficients of the monomials are shown, along with their alternating sums (fixed , alternation over ). The squares with yellow highlighting are those on the "critical diagonals", where or , where Data:Rolfsen Splice Base/Signature is the signature of Rolfsen Splice Base. Nonzero entries off the critical diagonals (if any exist) are highlighted in red. | Data:Rolfsen Splice Base/KhovanovTable |
Integral Khovanov Homology
(db, data source) |
Data:Rolfsen Splice Base/Integral Khovanov Homology |
The Coloured Jones Polynomials
2 | <*ColouredJones[K, 2][q]*> |
3 | <*ColouredJones[K, 3][q]*> |
4 | <*ColouredJones[K, 4][q]*> |
5 | <*ColouredJones[K, 5][q]*> |
6 | <*ColouredJones[K, 6][q]*> |
7 | <*ColouredJones[K, 7][q]*> |
Computer Talk
Much of the above data can be recomputed by Mathematica using the package KnotTheory`
. See A Sample KnotTheory` Session.
Template:Computer Talk
See/edit the Rolfsen_Splice_Template.
Back to the top. |
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<* (* *) *>