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Cycles of many lengths in Hamiltonian graphs

Published online by Cambridge University Press:  31 August 2022

Matija Bucić
Affiliation:
Institute for Advanced Study and Princeton University, Washington Road, Fine Hall, US-08544 Princeton, USA; E-mail: matija.bucic@ias.edu.
Lior Gishboliner
Affiliation:
Department of Mathematics, ETH, Zürich, Rämistrasse 101, Zürich, CH-8092, Switzerland; E-mail: lior.gishboliner@math.ethz.ch.
Benny Sudakov
Affiliation:
Department of Mathematics, ETH, Zürich, Rämistrasse 101, Zürich, CH-8092, Switzerland; E-mail: benjamin.sudakov@math.ethz.ch.

Abstract

In 1999, Jacobson and Lehel conjectured that, for $k \geq 3$, every k-regular Hamiltonian graph has cycles of $\Theta (n)$ many different lengths. This was further strengthened by Verstraëte, who asked whether the regularity can be replaced with the weaker condition that the minimum degree is at least $3$. Despite attention from various researchers, until now, the best partial result towards both of these conjectures was a $\sqrt {n}$ lower bound on the number of cycle lengths. We resolve these conjectures asymptotically by showing that the number of cycle lengths is at least $n^{1-o(1)}$.

Information

Type
Discrete Mathematics
Creative Commons
Creative Common License - CCCreative Common License - BYCreative Common License - NCCreative Common License - ND
This is an Open Access article, distributed under the terms of the Creative Commons Attribution-NonCommercial-NoDerivatives licence (https://creativecommons.org/licenses/by-nc-nd/4.0/), which permits non-commercial re-use, distribution, and reproduction in any medium, provided the original work is unaltered and is properly cited. The written permission of Cambridge University Press must be obtained for commercial re-use or in order to create a derivative work.
Copyright
© The Author(s), 2022. Published by Cambridge University Press
Figure 0

Figure 1 A section pair with a chord $(x,y)$ and its corresponding trivial path marked in red.

Figure 1

Figure 2 A parallel collection of subsection pairs.

Figure 2

Figure 3 An interlacing collection of subsection pairs.

Figure 3

Figure 4 Different paths $P^{\prime }_i$.

Figure 4

Figure 5 A combination of $P_2'$ and a path provided by induction (marked as zigzag in the figure).

Figure 5

Figure 6 $Q_1^R,Q_2^R$ are marked as red zigzag paths, $Q^{\prime }_R$ is depicted in red, $Q_1^B,Q_2^B$ are marked as blue zigzag paths, $Q^{\prime }_B$ is depicted in blue and some $R_i$ is depicted in green.

Figure 6

Figure 7 The lower part of the path is provided by the induction and can be chosen among $\tilde {\Omega }(m^{i\varepsilon })$ paths with lengths in an interval of size $m^{i\varepsilon }$. The upper top-bottom path-pair for $X_{i+1},Y_{i+1}$ can be chosen among a collection of $\tilde {\Omega }(m^{\varepsilon })$ of them with lengths $m^{i\varepsilon }$ apart.

Figure 7

Figure 8 Case 1 of Lemma 4.2. Note that trivial paths using any two distinct edges of a star always have different lengths.

Figure 8

Figure 9 Case 2 of Lemma 4.2. Edges $(x_j,y_j)$ are depicted in red. Shaded regions have many chords and will become $X_j^{\prime \prime },Y_j^{\prime \prime }$.

Figure 9

Figure 10 Two options for how $(x_j,y_j)$ can interlace $X_j^{\prime \prime },Y_j^{\prime \prime }$ and the corresponding top-bottom path-pairs we use.

Figure 10

Figure 11 Rerouting through a path $B^{\prime }_i$ marked in red.

Figure 11

Figure 12 Rerouted path $B^{\prime }_i$ with new relative positions of the section pairs.