T(11,3)

T(21,2)

T(23,2)

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	Edit T(11,3) Quick Notes

Edit T(11,3) Further Notes and Views

Knot presentations

Planar diagram presentation	X7,37,8,36 X22,38,23,37 X23,9,24,8 X38,10,39,9 X39,25,40,24 X10,26,11,25 X11,41,12,40 X26,42,27,41 X27,13,28,12 X42,14,43,13 X43,29,44,28 X14,30,15,29 X15,1,16,44 X30,2,31,1 X31,17,32,16 X2,18,3,17 X3,33,4,32 X18,34,19,33 X19,5,20,4 X34,6,35,5 X35,21,36,20 X6,22,7,21
Gauss code	14, -16, -17, 19, 20, -22, -1, 3, 4, -6, -7, 9, 10, -12, -13, 15, 16, -18, -19, 21, 22, -2, -3, 5, 6, -8, -9, 11, 12, -14, -15, 17, 18, -20, -21, 1, 2, -4, -5, 7, 8, -10, -11, 13
Dowker-Thistlethwaite code	30 -32 34 -36 38 -40 42 -44 2 -4 6 -8 10 -12 14 -16 18 -20 22 -24 26 -28

Braid presentation

Polynomial invariants

Alexander polynomial	$t^{10}-t^{9}+t^{7}-t^{6}+t^{4}-t^{3}+t-1+t^{-1}-t^{-3}+t^{-4}-t^{-6}+t^{-7}-t^{-9}+t^{-10}$
Conway polynomial	$z^{20}+19z^{18}+152z^{16}+666z^{14}+1742z^{12}+2782z^{10}+2665z^{8}+1443z^{6}+390z^{4}+40z^{2}+1$
2nd Alexander ideal (db, data sources)	$\{1\}$
Determinant and Signature	{ 1, 16 }
Jones polynomial	$-q^{22}+q^{12}+q^{10}$
HOMFLY-PT polynomial (db, data sources)	$z^{20}a^{-20}+20z^{18}a^{-20}-z^{18}a^{-22}+171z^{16}a^{-20}-19z^{16}a^{-22}+817z^{14}a^{-20}-152z^{14}a^{-22}+z^{14}a^{-24}+2394z^{12}a^{-20}-666z^{12}a^{-22}+14z^{12}a^{-24}+4446z^{10}a^{-20}-1742z^{10}a^{-22}+78z^{10}a^{-24}+5226z^{8}a^{-20}-2782z^{8}a^{-22}+221z^{8}a^{-24}+3770z^{6}a^{-20}-2665z^{6}a^{-22}+338z^{6}a^{-24}+1560z^{4}a^{-20}-1443z^{4}a^{-22}+273z^{4}a^{-24}+325z^{2}a^{-20}-390z^{2}a^{-22}+105z^{2}a^{-24}+26a^{-20}-40a^{-22}+15a^{-24}$
Kauffman polynomial (db, data sources)	Data:T(11,3)/Kauffman Polynomial
The A2 invariant	Data:T(11,3)/QuantumInvariant/A2/1,0
The G2 invariant	Data:T(11,3)/QuantumInvariant/G2/1,0

Further Quantum Invariants[show]

T(11,3) Quantum Invariants.

Computer Talk[show]

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. Read more at http://katlas.math.toronto.edu/wiki/KnotTheory.

In[3]:=

K = Knot["T(11,3)"];

In[4]:=

Alexander[K][t]

KnotTheory::loading: Loading precomputed data in PD4Knots`.

Out[4]=

$t^{10}-t^{9}+t^{7}-t^{6}+t^{4}-t^{3}+t-1+t^{-1}-t^{-3}+t^{-4}-t^{-6}+t^{-7}-t^{-9}+t^{-10}$

In[5]:=

Conway[K][z]

Out[5]=

$z^{20}+19z^{18}+152z^{16}+666z^{14}+1742z^{12}+2782z^{10}+2665z^{8}+1443z^{6}+390z^{4}+40z^{2}+1$

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]=

{ 1, 16 }

In[8]:=

Jones[K][q]

KnotTheory::loading: Loading precomputed data in Jones4Knots`.

Out[8]=

$-q^{22}+q^{12}+q^{10}$

In[9]:=

HOMFLYPT[K][a, z]

KnotTheory::credits: The HOMFLYPT program was written by Scott Morrison.

Out[9]=

$z^{20}a^{-20}+20z^{18}a^{-20}-z^{18}a^{-22}+171z^{16}a^{-20}-19z^{16}a^{-22}+817z^{14}a^{-20}-152z^{14}a^{-22}+z^{14}a^{-24}+2394z^{12}a^{-20}-666z^{12}a^{-22}+14z^{12}a^{-24}+4446z^{10}a^{-20}-1742z^{10}a^{-22}+78z^{10}a^{-24}+5226z^{8}a^{-20}-2782z^{8}a^{-22}+221z^{8}a^{-24}+3770z^{6}a^{-20}-2665z^{6}a^{-22}+338z^{6}a^{-24}+1560z^{4}a^{-20}-1443z^{4}a^{-22}+273z^{4}a^{-24}+325z^{2}a^{-20}-390z^{2}a^{-22}+105z^{2}a^{-24}+26a^{-20}-40a^{-22}+15a^{-24}$

In[10]:=

Kauffman[K][a, z]

KnotTheory::loading: Loading precomputed data in Kauffman4Knots`.

Out[10]=

Data:T(11,3)/Kauffman Polynomial

"Similar" Knots (within the Atlas)

Same Alexander/Conway Polynomial: {}

Same Jones Polynomial (up to mirroring, $q\leftrightarrow q^{-1}$): {}

Computer Talk[show]

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. Read more at http://katlas.math.toronto.edu/wiki/KnotTheory.

In[3]:=

K = Knot["T(11,3)"];

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]=

{ $t^{10}-t^{9}+t^{7}-t^{6}+t^{4}-t^{3}+t-1+t^{-1}-t^{-3}+t^{-4}-t^{-6}+t^{-7}-t^{-9}+t^{-10}$, $-q^{22}+q^{12}+q^{10}$ }

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]=

{}

Vassiliev invariants

V2 and V3:

(40, 220)

V2,1 through V6,9:

V2,1 V3,1 V4,1 V4,2 V4,3 V5,1 V5,2 V5,3 V5,4 V6,1 V6,2 V6,3 V6,4 V6,5 V6,6 V6,7 V6,8 V6,9 Data:T(11,3)/V 2,1 Data:T(11,3)/V 3,1 Data:T(11,3)/V 4,1 Data:T(11,3)/V 4,2 Data:T(11,3)/V 4,3 Data:T(11,3)/V 5,1 Data:T(11,3)/V 5,2 Data:T(11,3)/V 5,3 Data:T(11,3)/V 5,4 Data:T(11,3)/V 6,1 Data:T(11,3)/V 6,2 Data:T(11,3)/V 6,3 Data:T(11,3)/V 6,4 Data:T(11,3)/V 6,5 Data:T(11,3)/V 6,6 Data:T(11,3)/V 6,7 Data:T(11,3)/V 6,8 Data:T(11,3)/V 6,9

V_2,1 through V_6,9 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 $t^{r}q^{j}$ are shown, along with their alternating sums $\chi$ (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=$16 is the signature of T(11,3). Nonzero entries off the critical diagonals (if any exist) are highlighted in red.

\   r    \    j   \ 0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 χ 45                               1 -1 43                           1     -1 41                           1 1   0 39                       1 1       0 37                   1     1       0 35                   1 1           0 33               1 1               0 31           1     1               0 29           1 1                   0 27       1 1                       0 25         1                       1 23     1                           1 21 1                               1 19 1                               1

Integral Khovanov Homology (db, data source)

$\dim {\mathcal {G}}_{2r+i}\operatorname {KH} _{\mathbb {Z} }^{r}$ $i=13$ $i=15$ $i=17$ $i=19$ $i=21$ $r=0$ ${\mathbb {Z} }$ ${\mathbb {Z} }$ $r=1$ $r=2$ ${\mathbb {Z} }$ $r=3$ ${\mathbb {Z} }_{2}$ ${\mathbb {Z} }$ $r=4$ ${\mathbb {Z} }$ ${\mathbb {Z} }$ $r=5$ ${\mathbb {Z} }$ ${\mathbb {Z} }$ $r=6$ ${\mathbb {Z} }$ $r=7$ ${\mathbb {Z} }_{2}$ ${\mathbb {Z} }$ $r=8$ ${\mathbb {Z} }$ ${\mathbb {Z} }$ $r=9$ ${\mathbb {Z} }$ ${\mathbb {Z} }$ $r=10$ ${\mathbb {Z} }$ $r=11$ ${\mathbb {Z} }_{2}$ ${\mathbb {Z} }$ $r=12$ ${\mathbb {Z} }$ ${\mathbb {Z} }$ $r=13$ ${\mathbb {Z} }$ ${\mathbb {Z} }$ $r=14$ ${\mathbb {Z} }$ $r=15$ ${\mathbb {Z} }_{2}$ ${\mathbb {Z} }$

Computer Talk

Much of the above data can be recomputed by Mathematica using the package KnotTheory`. See A Sample KnotTheory` Session.

Modifying This Page

Read me first: Modifying Knot Pages See/edit the Torus Knot Page master template (intermediate). See/edit the Torus Knot_Splice_Base (expert). Back to the top.

T(21,2) T(23,2)