L7a4

L7a3

L7a5

	Visit L7a4's page at Knotilus! Visit L7a4's page at the original Knot Atlas!
	L7a4 is $7_{3}^{2}$ in the Rolfsen table of links.

L7a4 Further Notes and Views

Knot presentations

Planar diagram presentation	X6172 X10,4,11,3 X14,8,5,7 X12,10,13,9 X8,14,9,13 X2536 X4,12,1,11
Gauss code	{1, -6, 2, -7}, {6, -1, 3, -5, 4, -2, 7, -4, 5, -3}

Polynomial invariants

Multivariable Alexander Polynomial (in $u$, $v$, $w$, ...)	$-{\frac {2(u-1)(v-1)}{{\sqrt {u}}{\sqrt {v}}}}$ (db)
Jones polynomial	$-2q^{9/2}+2q^{7/2}-3q^{5/2}+3q^{3/2}-{\frac {1}{q^{3/2}}}+q^{11/2}-3{\sqrt {q}}+{\frac {1}{\sqrt {q}}}$ (db)
Signature	1 (db)
HOMFLY-PT polynomial	$-z^{3}a^{-1}-z^{3}a^{-3}+az-za^{-1}-za^{-3}+za^{-5}+az^{-1}-a^{-1}z^{-1}$ (db)
Kauffman polynomial	$-z^{6}a^{-2}-z^{6}a^{-4}-z^{5}a^{-1}-3z^{5}a^{-3}-2z^{5}a^{-5}+z^{4}a^{-2}+z^{4}a^{-4}-z^{4}a^{-6}-z^{4}-az^{3}-z^{3}a^{-1}+5z^{3}a^{-3}+5z^{3}a^{-5}-2z^{2}a^{-2}+2z^{2}a^{-6}+2az+2za^{-1}-2za^{-3}-2za^{-5}+1-az^{-1}-a^{-1}z^{-1}$ (db)

Vassiliev invariants

V2 and V3:

(0, -1)

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:L7a4/V 2,1 Data:L7a4/V 3,1 Data:L7a4/V 4,1 Data:L7a4/V 4,2 Data:L7a4/V 4,3 Data:L7a4/V 5,1 Data:L7a4/V 5,2 Data:L7a4/V 5,3 Data:L7a4/V 5,4 Data:L7a4/V 6,1 Data:L7a4/V 6,2 Data:L7a4/V 6,3 Data:L7a4/V 6,4 Data:L7a4/V 6,5 Data:L7a4/V 6,6 Data:L7a4/V 6,7 Data:L7a4/V 6,8 Data:L7a4/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=$1 is the signature of L7a4. Nonzero entries off the critical diagonals (if any exist) are highlighted in red.

\   r    \    j   \ -2 -1 0 1 2 3 4 5 χ 12               1 -1 10             1   1 8           1 1   0 6         2 1     1 4       1 1       0 2     2 2         0 0   1 3           2 -2                 0 -4 1               1

Integral Khovanov Homology (db, data source)

$\dim {\mathcal {G}}_{2r+i}\operatorname {KH} _{\mathbb {Z} }^{r}$ $i=0$ $i=2$ $r=-2$ ${\mathbb {Z} }$ $r=-1$ ${\mathbb {Z} }_{2}$ ${\mathbb {Z} }$ $r=0$ ${\mathbb {Z} }^{3}$ ${\mathbb {Z} }^{2}$ $r=1$ ${\mathbb {Z} }^{2}\oplus {\mathbb {Z} }_{2}$ ${\mathbb {Z} }$ $r=2$ ${\mathbb {Z} }\oplus {\mathbb {Z} }_{2}^{2}$ ${\mathbb {Z} }^{2}$ $r=3$ ${\mathbb {Z} }\oplus {\mathbb {Z} }_{2}$ ${\mathbb {Z} }$ $r=4$ ${\mathbb {Z} }\oplus {\mathbb {Z} }_{2}$ ${\mathbb {Z} }$ $r=5$ ${\mathbb {Z} }_{2}$ ${\mathbb {Z} }$

Computer Talk

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

${\textrm {Include}}({\textrm {ColouredJonesM.mhtml}})$

In[1]:=	<< KnotTheory`
Loading KnotTheory` (version of August 17, 2005, 14:44:34)...
In[2]:=	Crossings[Link[7, Alternating, 4]]
Out[2]=	7
In[3]:=	PD[Link[7, Alternating, 4]]
Out[3]=	PD[X[6, 1, 7, 2], X[10, 4, 11, 3], X[14, 8, 5, 7], X[12, 10, 13, 9], X[8, 14, 9, 13], X[2, 5, 3, 6], X[4, 12, 1, 11]]
In[4]:=	GaussCode[Link[7, Alternating, 4]]
Out[4]=	GaussCode[{1, -6, 2, -7}, {6, -1, 3, -5, 4, -2, 7, -4, 5, -3}]
In[5]:=	BR[Link[7, Alternating, 4]]
Out[5]=	BR[Link[7, Alternating, 4]]
In[6]:=	alex = Alexander[Link[7, Alternating, 4]][t]
Out[6]=	ComplexInfinity
In[7]:=	Conway[Link[7, Alternating, 4]][z]
Out[7]=	ComplexInfinity
In[8]:=	Select[AllKnots[], (alex === Alexander[#][t])&]
Out[8]=	{}
In[9]:=	{KnotDet[Link[7, Alternating, 4]], KnotSignature[Link[7, Alternating, 4]]}
Out[9]=	{Infinity, 1}
In[10]:=	J=Jones[Link[7, Alternating, 4]][q]
Out[10]=	-(3/2) 1 3/2 5/2 7/2 9/2 -q + ------- - 3 Sqrt[q] + 3 q - 3 q + 2 q - 2 q + Sqrt[q] 11/2 q
In[11]:=	Select[AllKnots[], (J === Jones[#][q] || (J /. q-> 1/q) === Jones[#][q])&]
Out[11]=	{}
In[12]:=	A2Invariant[Link[7, Alternating, 4]][q]
Out[12]=	-6 -4 -2 2 4 10 14 18 3 + q + q + q + q + q + q + q - q
In[13]:=	Kauffman[Link[7, Alternating, 4]][a, z]
Out[13]=	2 2 3 3 1 a 2 z 2 z 2 z 2 z 2 z 5 z 5 z 1 - --- - - - --- - --- + --- + 2 a z + ---- - ---- + ---- + ---- - a z z 5 3 a 6 2 5 3 a a a a a a 3 4 4 4 5 5 5 6 6 z 3 4 z z z 2 z 3 z z z z -- - a z - z - -- + -- + -- - ---- - ---- - -- - -- - -- a 6 4 2 5 3 a 4 2 a a a a a a a
In[14]:=	{Vassiliev[2][Link[7, Alternating, 4]], Vassiliev[3][Link[7, Alternating, 4]]}
Out[14]=	{0, -1}
In[15]:=	Kh[Link[7, Alternating, 4]][q, t]
Out[15]=	2 1 1 2 4 4 2 6 2 6 3 3 + 2 q + ----- + - + 2 q t + q t + q t + 2 q t + q t + 4 2 t q t 8 3 8 4 10 4 12 5 q t + q t + q t + q t