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A pair degree condition for Hamiltonian cycles in 3-uniform hypergraphs

Published online by Cambridge University Press:  17 May 2023

Bjarne Schülke*
Affiliation:
Department of Mathematics, University of Hamburg, Hamburg, Germany Department of Mathematics, California Institute of Technology, Pasadena, CA, USA
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Abstract

We prove a new sufficient pair degree condition for tight Hamiltonian cycles in $3$-uniform hypergraphs that (asymptotically) improves the best known pair degree condition due to Rödl, Ruciński, and Szemerédi. For graphs, Chvátal characterised all those sequences of integers for which every pointwise larger (or equal) degree sequence guarantees the existence of a Hamiltonian cycle. A step towards Chvátal’s theorem was taken by Pósa, who improved on Dirac’s tight minimum degree condition for Hamiltonian cycles by showing that a certain weaker condition on the degree sequence of a graph already yields a Hamiltonian cycle.

In this work, we take a similar step towards a full characterisation of all pair degree matrices that ensure the existence of tight Hamiltonian cycles in $3$-uniform hypergraphs by proving a $3$-uniform analogue of Pósa’s result. In particular, our result strengthens the asymptotic version of the result by Rödl, Ruciński, and Szemerédi.

MSC classification

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Paper
Creative Commons
Creative Common License - CCCreative Common License - BYCreative Common License - NCCreative Common License - SA
This is an Open Access article, distributed under the terms of the Creative Commons Attribution-NonCommercial-ShareAlike licence (https://creativecommons.org/licenses/by-nc-sa/4.0/), which permits non-commercial re-use, distribution, and reproduction in any medium, provided the same Creative Commons licence is included and the original work is properly cited. The written permission of Cambridge University Press must be obtained for commercial re-use.
Copyright
© The Author(s), 2023. Published by Cambridge University Press
Figure 0

Figure 1. Overview of the proof.

Figure 1

Figure 2. Idea of the second step, the picture is similar to [16, Fig. 4.1].

Figure 2

Figure 3. Structure of the absorbers with hyperedges used before absorption of $x$ in dark red and hyperedges used after absorption of $x$ in light red.