ropelength

{{short description|Knot invariant}}

In physical knot theory, each realization of a link or knot has an associated ropelength. Intuitively this is the minimal length of an ideally flexible rope that is needed to tie a given link, or knot. Knots and links that minimize ropelength are called ideal knots and ideal links respectively.

Image:Ideal Trefoil.png.]]

Definition

The ropelength of a knotted curve C is defined as the ratio L(C) = \operatorname{Len}(C)/\tau(C), where \operatorname{Len}(C) is the length of C and \tau(C) is the knot thickness of C.

Ropelength can be turned into a knot invariant by defining the ropelength of a knot K to be the minimum ropelength over all curves that realize K.

Ropelength minimizers

One of the earliest knot theory questions was posed in the following terms:

{{block indent|left=1.6|Can I tie a knot on a foot-long rope that is one inch thick?}}

In terms of ropelength, this asks if there is a knot with ropelength 12. The answer is no: an argument using quadrisecants shows that the ropelength of any nontrivial knot has to be at least 15.66.{{r|DDS}} However, the search for the answer has spurred research on both theoretical and computational ground. It has been shown that for each link type there is a ropelength minimizer although it may only be of differentiability class C^1.{{r|GMSV|CKS}} For the simplest nontrivial knot, the trefoil knot, computer simulations have shown that its minimum ropelength is at most 16.372.{{r|DDS}}

Dependence on crossing number

An extensive search has been devoted to showing relations between ropelength and other knot invariants such as the crossing number of a knot. For every knot K, the ropelength of K is at least proportional to \operatorname{Cr}(K)^{3/4}, where \operatorname{Cr}(K) denotes the crossing number.{{r|BS}} There exist knots and links, namely the (k,k-1) torus knots and k-Hopf links, for which this lower bound is tight. That is, for these knots (in big O notation),{{r|CKS}}

L(K)=O(\operatorname{Cr}(K)^{3/4}).

On the other hand, there also exist knots whose ropelength is larger, proportional to the crossing number itself rather than to a smaller power of it.{{r|DET}} This is nearly tight, as for every knot,

L(K)= O(\operatorname{Cr}(K)\log^5(\operatorname{Cr}(K))).

The proof of this near-linear upper bound uses a divide-and-conquer argument to show that minimum projections of knots can be embedded as planar graphs in the cubic lattice.{{r|DEPZ}} However, no one has yet observed a knot family with super-linear dependence of length on crossing number and it is conjectured that the tight upper bound should be linear.{{r|DE}}

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Category:Knot invariants

Category:Geometric topology