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Self-avoiding walk is ballistic on graphs with more than one end

Published online by Cambridge University Press:  28 October 2025

Florian Lehner
Affiliation:
University of Auckland , New Zealand; E-mail: florian.lehner@auckland.ac.nz
Christian Lindorfer
Affiliation:
Technische Universitat Graz , Austria; E-mail: chri.lindorfer@gmail.com
Christoforos Panagiotis*
Affiliation:
University of Bath , United Kingdom
*
E-mail: cp2324@bath.ac.uk (Corresponding author)

Abstract

We prove that on any transitive graph G with infinitely many ends, a self-avoiding walk of length n is ballistic with extremely high probability, in the sense that there exist constants $c,t>0$ such that $\mathbb {P}_n(d_G(w_0,w_n)\geq cn)\geq 1-e^{-tn}$ for every $n\geq 1$. Furthermore, we show that the number of self-avoiding walks of length n grows asymptotically like $\mu _w^n$, in the sense that there exists $C>0$ such that $\mu _w^n\leq c_n\leq C\mu _w^n$ for every $n\geq 1$. These results generalise earlier work by Li (J. Comb. Theory Ser. A, 2020). The key to this greater generality is that in contrast to Li’s approach, our proof does not require the existence of a special structure that enables the construction of separating patterns. Our results also extend more generally to quasi-transitive graphs with infinitely many ends, satisfying the additional technical property that there is a quasi-transitive group of automorphisms of G which does not fix an end of G.

Information

Type
Probability
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, provided the original article is properly cited.
Copyright
© The Author(s), 2025. Published by Cambridge University Press
Figure 0

Figure 1 A self-avoiding walk and its decomposition into configurations and shapes. Note that every edge of the graph appears in exactly one part. Dashed edges correspond to detours whose edges do not lie in this part; configurations also keep track on which side the detour lies on. The little arrows pointing in and out of every configuration indicate the side on which the first and last edge of the self-avoiding walk lie, respectively.

Figure 1

Figure 2 A complete arrangement. Virtual edges in part graphs and adhesion graphs are drawn in gray and are dashed in the paths making up the arrangement. The little arrows indicate entry and exit directions: the shaft of the arrow pointing into e points towards $X(e)$, the tip of the arrow pointing out of e points towards $Y(e)$.

Figure 2

Figure 3 Four arrangements on $\mathrm {star}(t_1)$ only differing in their entry and exit directions. The arrangement in the top left corner is complete, the others are not. Note that the shapes on $t_2$ which can be used to extend the incomplete arrangements (that is, shapes on $t_2$ compatible with the respective configurations on $e_2$) are different.

Figure 3

Figure 4 Example of contraction (see Construction 4.5) and projection (see Construction 4.8) of arrangements with respect to the arc f. Note that virtual edges in $\mathcal {E}(f)$ and $\mathcal {E}(\bar f)$ are no longer present in the part graph after contraction.

Figure 4

Figure 5 A c-completion. Note that this is not a complete configuration; it is, however, ‘almost’ complete in the sense that the only nonboring configuration in the boundary is c.

Figure 5

Figure 6 A c-$c'$-completion of length 2. Note that there are two boundary arcs (the source arc and target arc) with nonboring configurations c and $c'$, respectively. In this example there are no other boundary arcs, but in general, configurations on all other boundary arcs would have to be boring.

Figure 6

Figure 7 Completions of an I-configuration (left) and U-configuration (right). Note that the walk corresponding to a completion of a U-configuration must return to the adhesion set, thus forming a U-shape.

Figure 7

Figure 8 Reflection-extension with splitting point u. The last part of the original walk is drawn in grey; the modified walk is drawn in black. Note that the distance between $u'$ and $g_e(u')$ is bounded by an absolute constant, so the increase in length will become negligible when the length of the original walk is large.