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Graphing, homotopy groups of spheres, and spaces of long links and knots

Published online by Cambridge University Press:  12 February 2025

Robin Koytcheff*
Affiliation:
Department of Mathematics, University of Louisiana at Lafayette, Lafayette, 70504 LA, USA

Abstract

We study homotopy groups of spaces of long links in Euclidean space of codimension at least three. With multiple components, they admit split injections from homotopy groups of spheres. We show that, up to knotting, these account for all the homotopy groups in a range which depends on the dimensions of the source manifolds and target manifold and which roughly generalizes the triple-point-free range for isotopy classes. Just beyond this range, joining components sends both a parametrized long Borromean rings class and a Hopf fibration to a generator of the first nontrivial homotopy group of the space of long knots. For spaces of equidimensional long links of most source dimensions, we describe generators for the homotopy group in this degree in terms of these Borromean rings and homotopy groups of spheres. A key ingredient in most of our results is a graphing map which increases source and target dimensions by one.

Information

Type
Topology
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution, and reproduction in any medium, provided the original work is properly cited.
Copyright
© The Author(s), 2025. Published by Cambridge University Press
Figure 0

Figure 1 Picture of the long Borromean rings (i.e., a pure braid commutator) $[b_{21},b_{31}]$ and the results of joining its components in the classical setting where $p=1$ and $n=3$.

Figure 1

Figure 2 (a) The singular 3-strand braid $f=(f_1,f_2,f_3)$ used to build the family F. (b) The singular 3-strand braid $f'=(f_1^{\prime },f_2^{\prime },f_3^{\prime })$ used to build the family $F'$.

Figure 2

Figure 3 The singular 2-component long link $\ell =(\ell _1, \ell _2)$obtained by joining strand 2 to strand 3 in the singular braid $f=(f_1,f_2,f_3)$. An isotopy takes this singular long link to a singular 2-strand pure braid.

Figure 3

Figure 4 The singular 2-component long link $\ell '=(\ell _1^{\prime }, \ell _2^{\prime })$ obtained by joining strand 2 to strand 3 in the singular braid $f'=(f^{\prime }_1,f^{\prime }_2,f^{\prime }_3)$.

Figure 4

Figure 5 The singular 2-component braid $h=(h_1,h_2)$ used to construct the family H.

Figure 5

Figure 6 The singular knot k obtained by joining the two components of the singular 2-component braid h.

Figure 6

Figure 7 The singular knot obtained by joining the two components of the singular link $\ell ' =(\ell _1^{\prime }, \ell _2^{\prime })$.