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Visit 5 1's page at the Knot Server (KnotPlot driven, includes 3D interactive images!)
Visit 5 1's page at Knotilus!
Visit 5 1's page at the original Knot Atlas!
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An interlaced pentagram, this is known variously as the "Cinquefoil Knot", after certain herbs and shrubs of the rose family which have 5-lobed leaves and 5-petaled flowers (see e.g. [4]),
as the "Pentafoil Knot" (visit Bert Jagers' pentafoil page),
as the "Double Overhand Knot", as 5_1, or finally as the torus knot T(5,2).
When taken off the post the strangle knot (hitch) of practical knot tying deforms to 5_1
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A kolam of a 2x3 dot array
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The VISA Interlink Logo [1]
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A pentagonal table by Bob Mackay [2]
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The Utah State Parks logo
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As impossible object ("Penrose" pentagram)
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Folded ribbon which is single-sided (more complex version of Möbius Strip).
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Alternate pentagram of intersecting circles.
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Partial view of US bicentennial logo on a shirt seen in Lisboa [3]
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Non-prime knot with two 5_1 configurations on a closed loop.
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Sum of two 5_1s, Vienna, orthodox church
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This sentence was last edited by Dror.
Sometime later, Scott added this sentence.
Knot presentations
Planar diagram presentation
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X1627 X3849 X5,10,6,1 X7283 X9,4,10,5
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Gauss code
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-1, 4, -2, 5, -3, 1, -4, 2, -5, 3
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Dowker-Thistlethwaite code
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6 8 10 2 4
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Conway Notation
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[5]
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Four dimensional invariants
Polynomial invariants
Alexander polynomial |
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Conway polynomial |
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2nd Alexander ideal (db, data sources) |
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Determinant and Signature |
{ 5, -4 } |
Jones polynomial |
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HOMFLY-PT polynomial (db, data sources) |
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Kauffman polynomial (db, data sources) |
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The A2 invariant |
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The G2 invariant |
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Further Quantum Invariants
Further quantum knot invariants for 5_1.
A1 Invariants.
Weight
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Invariant
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1
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2
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3
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4
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5
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6
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8
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A2 Invariants.
Weight
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Invariant
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1,0
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1,1
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2,0
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3,0
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A3 Invariants.
Weight
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Invariant
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0,1,0
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1,0,0
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1,0,1
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A4 Invariants.
Weight
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Invariant
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0,1,0,0
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1,0,0,0
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B2 Invariants.
Weight
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Invariant
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0,1
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1,0
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B3 Invariants.
Weight
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Invariant
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1,0,0
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B4 Invariants.
Weight
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Invariant
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1,0,0,0
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C3 Invariants.
Weight
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Invariant
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1,0,0
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C4 Invariants.
Weight
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Invariant
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1,0,0,0
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D4 Invariants.
Weight
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Invariant
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0,1,0,0
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1,0,0,0
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G2 Invariants.
Weight
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Invariant
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0,1
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1,0
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.
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]:=
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AppendTo[$Path, "C:/drorbn/projects/KAtlas/"];
<< KnotTheory`
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KnotTheory::loading: Loading precomputed data in PD4Knots`.
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Out[4]=
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Out[5]=
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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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In[7]:=
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{KnotDet[K], KnotSignature[K]}
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KnotTheory::loading: Loading precomputed data in Jones4Knots`.
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Out[8]=
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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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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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V2,1 through V6,9:
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V2,1
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V3,1
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V4,1
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V4,2
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V4,3
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V5,1
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V5,2
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V5,3
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V5,4
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V6,1
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V6,2
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V6,3
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V6,4
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V6,5
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V6,6
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V6,7
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V6,8
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V6,9
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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.
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 -4 is the signature of 5 1. Nonzero entries off the critical diagonals (if any exist) are highlighted in red.
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-5 | -4 | -3 | -2 | -1 | 0 | χ |
-3 | | | | | | 1 | 1 |
-5 | | | | | | 1 | 1 |
-7 | | | | 1 | | | 1 |
-9 | | | | | | | 0 |
-11 | | 1 | 1 | | | | 0 |
-13 | | | | | | | 0 |
-15 | 1 | | | | | | -1 |
Computer Talk
Much of the above data can be recomputed by Mathematica using the package KnotTheory`
. See A Sample KnotTheory` Session.
In[1]:= |
<< KnotTheory` |
Loading KnotTheory` (version of August 17, 2005, 14:44:34)... |
In[2]:= | Crossings[Knot[5, 1]] |
Out[2]= | 5 |
In[3]:= | PD[Knot[5, 1]] |
Out[3]= | PD[X[1, 6, 2, 7], X[3, 8, 4, 9], X[5, 10, 6, 1], X[7, 2, 8, 3],
X[9, 4, 10, 5]] |
In[4]:= | GaussCode[Knot[5, 1]] |
Out[4]= | GaussCode[-1, 4, -2, 5, -3, 1, -4, 2, -5, 3] |
In[5]:= | BR[Knot[5, 1]] |
Out[5]= | BR[2, {-1, -1, -1, -1, -1}] |
In[6]:= | alex = Alexander[Knot[5, 1]][t] |
Out[6]= | -2 1 2
1 + t - - - t + t
t |
In[7]:= | Conway[Knot[5, 1]][z] |
Out[7]= | 2 4
1 + 3 z + z |
In[8]:= | Select[AllKnots[], (alex === Alexander[#][t])&] |
Out[8]= | {Knot[5, 1], Knot[10, 132]} |
In[9]:= | {KnotDet[Knot[5, 1]], KnotSignature[Knot[5, 1]]} |
Out[9]= | {5, -4} |
In[10]:= | J=Jones[Knot[5, 1]][q] |
Out[10]= | -7 -6 -5 -4 -2
-q + q - q + q + q |
In[11]:= | Select[AllKnots[], (J === Jones[#][q] || (J /. q-> 1/q) === Jones[#][q])&] |
Out[11]= | {Knot[5, 1], Knot[10, 132]} |
In[12]:= | A2Invariant[Knot[5, 1]][q] |
Out[12]= | -22 -20 -18 -14 -12 2 -8 -6
-q - q - q + q + q + --- + q + q
10
q |
In[13]:= | Kauffman[Knot[5, 1]][a, z] |
Out[13]= | 4 6 5 7 9 4 2 6 2 8 2
3 a + 2 a - 2 a z - a z + a z - 4 a z - 3 a z + a z +
5 3 7 3 4 4 6 4
a z + a z + a z + a z |
In[14]:= | {Vassiliev[2][Knot[5, 1]], Vassiliev[3][Knot[5, 1]]} |
Out[14]= | {0, -5} |
In[15]:= | Kh[Knot[5, 1]][q, t] |
Out[15]= | -5 -3 1 1 1 1
q + q + ------ + ------ + ------ + -----
15 5 11 4 11 3 7 2
q t q t q t q t |