L10a140 Link
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In the mathematical theory of knots, L10a140 is the name in th
Thistlethwaite link table
of a link of three loops, which has ten crossings between the loops when presented in its simplest visual form. It is of interest because it is presumably the simplest link which possesses the Brunnian property — a link of connected components that, when one component is removed, becomes entirely unconnected — other than the six-crossing Borromean rings. In other words, no two loops are directly linked with each other, but all three are collectively interlinked, so removing any loop frees the other two. In the image in the infobox at right, the red loop is not interlinked with either the blue or the yellow loops, and if the red loop is removed, then the blue and yellow loops can also be disentangled from each other without cutting either one. According to work by Slavik V. Jablan, the L10a140 link can be seen as the second in an infinite series of Brunnian links beginning with the Borromean rings. So if the blue and yellow loops have only one twist along each side, the resulting configuration is the Borromean rings; if the blue and yellow loops have three twists along each side, the resulting configuration is the L10a140 link; if the blue and yellow loops have five twists along each side, the resulting configuration is a three-loop link with 14 overall crossings, etc. etc.


Invariants

Th
multivariable Alexander polynomial
for the L10a140 link is : \Delta(u,v,w)=\frac, \, the Conway polynomial is : \nabla (z)=4z^4+4z^6+z^8, \, the Jones polynomial factors nicely as : \beginV(t) &= -t^5+3t^4-5t^3+8t^2-9t+12-9t^+8t^-5t^+3t^-t^ \\ pt& = -\frac\left(t^5-2 t^4+t^3-2t^2+t-1\right) \left(t^5-t^4+2 t^3-t^2+2t-1\right) \\ pt& = w(t) w(1/t), \, \end where w(t) = t^5-2 t^4+t^3-2 t^2+t-1. (Notice that w(t) is essentially the Jones polynomial for the
Whitehead link In knot theory, the Whitehead link, named for J. H. C. Whitehead, is one of the most basic links. It can be drawn as an alternating link with five crossings, from the overlay of a circle and a figure-eight shaped loop. Structure A common way ...
.) The
HOMFLY polynomial In the mathematical field of knot theory, the HOMFLY polynomial or HOMFLYPT polynomial, sometimes called the generalized Jones polynomial, is a 2-variable knot polynomial, i.e. a knot invariant in the form of a polynomial of variables ''m'' and ' ...
is : P(\alpha,z)=z^ \alpha^-4z^2 \alpha^-4z^4 \alpha^-z^6 \alpha^-2z^+8z^2+12z^4+6z^6+z^8+z^ \alpha^2-4z^2 \alpha^2-4z^4 \alpha^2-z^6 \alpha^2, \, and the Kauffman polynomial is : \begin F(a,z) & = 1 + 2z^ + a^z^ + a^z^ - 2a^z^ - az^ - 20z^2 + 2a^z^2 \\ pt& - 8a^z^2 - 8a^2 z^2 + 2a^4 z^4 + 2a^4 z^2 - 2a^ z^3 + 4a^ z^3 + 6a^ z^3 \\ pt& + 6az^3 +4a^3 z^3 - 2a^5 z^3 +42z^4 - 7a^ z^4 +14a^ z^ \\ pt& + 14a^2 z^4 -7a^4 z^4 + a^ z^ - 9a^z^5 - 2a^ z^5 - 2az^5 - 9a^3 z^5 \\ pt& + a^5 z^5 - 28z^6 +3a^ z^6 -11a^ z^6 -11a^2 z^6 + 3a^4 z^6 + 4a^ z^7 \\ pt& - 2a^ z^7 - 2az^7 + 4a^3 z^7 + 8z^8 + 4a^ z^8 + 4a^2 z^8 + 2a^ z^9 + 2az^9. \end


Pseudo-symmetric visual variants

David Swart, and independently Rick Mabry and Laura McCormick, discovered alternative 12-crossing visual representations of the L10a140 link. In these depictions, the link no longer has strictly alternating crossings (as it does in its simplest 10-crossing form), but there is greater superficial symmetry. So the leftmost image below shows a 12-crossing link (distinct from both the Borromean rings and the L10a140 link) with six-fold rotational symmetry. The center image shows a similar-looking depiction of the L10a140 link (but without true rotational symmetry). Similarly, the rightmost image shows a depiction of the L10a140 link with superficial fourfold symmetry. Image:Brunnian-3-not-Borromean.svg, Fully symmetrical 12-crossing Brunnian link (L12a1882) File:Marilyns Cross.gif, L10a140 in pseudo 6-symmetric form File:Marilyns Cross The Cross.gif, L10a140 in pseudo 4-symmetric form


References


External links


"It Is What It Is"
''Flickr.com''. {{Knot theory, state=collapsed Hyperbolic knots and links