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Continuous phase transitions on Galton–Watson trees

Published online by Cambridge University Press:  06 July 2021

Tobias Johnson*
Affiliation:
Department of Mathematics, College of Staten Island, Staten Island, NY 10314, USA
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Abstract

Distinguishing between continuous and first-order phase transitions is a major challenge in random discrete systems. We study the topic for events with recursive structure on Galton–Watson trees. For example, let $\mathcal{T}_1$ be the event that a Galton–Watson tree is infinite and let $\mathcal{T}_2$ be the event that it contains an infinite binary tree starting from its root. These events satisfy similar recursive properties: $\mathcal{T}_1$ holds if and only if $\mathcal{T}_1$ holds for at least one of the trees initiated by children of the root, and $\mathcal{T}_2$ holds if and only if $\mathcal{T}_2$ holds for at least two of these trees. The probability of $\mathcal{T}_1$ has a continuous phase transition, increasing from 0 when the mean of the child distribution increases above 1. On the other hand, the probability of $\mathcal{T}_2$ has a first-order phase transition, jumping discontinuously to a non-zero value at criticality. Given the recursive property satisfied by the event, we describe the critical child distributions where a continuous phase transition takes place. In many cases, we also characterise the event undergoing the phase transition.

Information

Type
Paper
Copyright
© The Author(s), 2021. Published by Cambridge University Press
Figure 0

Figure 1. Let $\chi_t$ be the probability measure placing the vector of probabilities $\bigl(\frac13-t,\,0,\,\frac12,\,\frac16+t\bigr)$ on values $0,\,1,\,2,\,3$. Let $h(0)=h(1)=h(2)=1$ and $h(3)=2$. The graphs above depict $\Psi_t(x)$, the automaton distribution map of $(\chi_t,h)$. The recursive tree system $(\chi_t,h)$ is critical at $t=0$ in the sense of Definition 1.4. As t increases, a single interpretable fixed point emerges and increases to 1 as t rises to $1/3$.

Figure 1

Figure 2. Graphs of $\Psi_t(x)-x$, where $\Psi_t$ is the automaton distribution map of $(\chi_t,h)$ with $\chi_t = \bigl(\frac{1}{20} - t\bigr)\delta_0 + \bigl(\frac12+t\bigr)\delta_2 + \frac{9}{20}\delta_5$, and $h(0)=h(2)=1$ and $h(5)=4$. The system $(\chi_t,h)$ is critical at $t=0$ in the sense of Definition 1.4, and we can see a fixed point emerging from 0 as t increases. Because $\Psi_t(x)\geq x$ in a neighbourhood of 0 for $t>0$, the interpretation associated with this fixed point is described in Theorem 1.8. See Example 1.8 for more details.

Figure 2

Figure 3. Graphs of $\Psi_t(x)-x$ illustrating a continuous phase transition not satisfying the conditions of Theorem 1.8. Here $\Psi_t$ is the automaton distribution map for $(\chi_t,h)$ where $\chi_t = \frac{1}{24}\delta_0 + \bigl(\frac12 - 3t^2\bigr)\delta_2 + \bigl(\frac16 + t\bigr)\delta_3 + \bigl(\frac{7}{24}+3t^2-t\bigr)\delta_6$, and $h(0)=h(2)=1$, $h(3)=2$, and $h(6)=5$. The top plot is our standard view of $\Psi_t(x)-x$ as in Figures 1 and 2. In the bottom plot, we zoom in around $x=0$ and see that two fixed points emerge from zero as t increases. By Proposition 1.1, the first fixed point for each system has no interpretation but the second one does. But we cannot apply Theorem 1.8 to characterise this interpretation. See Section 5 for further discussion.

Figure 3

Figure 4. Let $\chi$ place vector of probabilities $\bigl(\frac{1}{10},0,\frac12,\frac15,\frac15\bigr)$ on values 0, 1, 2, 3, 4, and let $h(0)=h(2)=1$ and $h(3)=h(4)=2$. The system $(\chi,h)$ is 2-supercordant; its automaton distribution map can be computed to be $\Psi(x)=x + \frac{13}{10}x^2 -2x^3 + \frac35 x^4$, with fixed point $x_0=(10-\sqrt{22})/6\approx 0.885$. The system $(\widetilde\chi,h)$ with the same fixed point but only a single value in tier 2 is found by computing $p=\varphi(x_0)\approx 0.406$, where $\varphi$ is given in (24), and then letting $\widetilde\chi$ place vector of probabilities $\bigl(\frac{1}{2}-p,0,\frac12,p,0\bigr)$ on 0, 1, 2, 3, 4. The automaton distribution map $\widetilde{\Psi}$ of $(\widetilde\chi,h)$ is shown above together with $\Psi$.

Figure 4

Figure 5. Graphs of $\Psi_t(x)-x$, where $\Psi_t$ is the automaton distribution map of $(\chi_t,h)$ with $\chi_t = \bigl(\frac{1}{2} + t\bigr)\delta_2 + \bigl(\frac12-t\bigr)\delta_3$, and $h(2)=1$ and $h(3)=3$. An interpretable fixed point emerges from 0 as t increases. The point 1 is a fixed point in all examples, and for $t\geq 1/6$ it is the only fixed point.