Regularity of Gibbs measures for unbounded spin systems on general graphs


Abstract

We consider a general class of spin systems with potentially unbounded real-valued spins, defined via a single-site potential with super-Gaussian tails on general graphs, allowing for both short- and long-range interactions. This class includes all \(P(\varphi)\) models, in particular the well-studied \(\varphi^4\) model. We construct an infinite-volume extremal measure called the plus measure as the limit of finite-volume Gibbs measures with weakly growing boundary conditions and show that it is regular, in the sense that it admits a bounded Radon-Nikodym derivative with respect to a product measure of single-site distributions with super-Gaussian tails. Moreover, we provide an alternative construction of the plus measure as the limit of finite-volume Gibbs measures that are regular up to the boundary.

As a key intermediate step, we establish regularity and tightness of finite-volume Gibbs measures for a large class of growing boundary conditions \(\xi\). Our regularity estimates are encoded in terms of a function \(A(\xi)\), which provides precise control on the change of measure induced by boundary perturbations, and can thus be viewed as an analogue of the Cameron–Martin theorem for non-Gaussian fields. In the nearest-neighbour case, this class includes boundary conditions that grow at most double-exponentially in the distance to the boundary when the single-site measure has tails of the form \(e^{-a|u|^n}\) for some \(n>2\). In contrast, when the single-site measure has Gaussian tails, the allowed growth is at most exponential. Our results apply to arbitrary graphs and improve upon earlier results of Lebowitz and Presutti [1], and Ruelle [2], [3], which apply in the context of \(\mathbb{Z}^d\) and allow only logarithmically growing boundary conditions, as well as subsequent extensions to vertex-transitive graphs of polynomial growth [4].

1 Introduction↩︎

We consider a general family of spin systems with pair interactions where each spin takes values in \(\mathbb{R}\). On a finite graph \((\Lambda, E)\) with ferromagnetic nearest-neighbour interactions and free boundary conditions, this consists of probability measures on spin configurations \(\varphi \in \mathbb{R}^{\Lambda}\) defined so that the expectation of a bounded measurable function \(f: \mathbb{R}^{\Lambda} \rightarrow \mathbb{R}\) is given by \[\langle f \rangle = \frac{1}{Z} \int_{\mathbb{R}^{\Lambda}} f(\varphi) \exp\left(\sum_{\{x,y\} \in E} \beta \varphi_x \varphi_y\right) \prod_{x \in \Lambda} \mathrm{d} \rho(\varphi_x),\] where \(\beta \geq 0\) is the inverse temperature, \(\rho\) is the single-site measure (chosen so that the above integral is finite), and \(Z\) is the appropriate normalisation constant, called the partition function. This framework includes several well-studied models in statistical physics:

  1. The Ising and \(\varphi^4\) models, by choosing, respectively \[\rho=\delta_{-1}+\delta_1, \qquad \mathrm{d}\rho(\varphi_x)=\exp(-g\varphi_x^4-a\varphi_x^2)\mathrm{d}\varphi_x,\] where for \(t\in \mathbb{R}\), \(\delta_t\) is the Dirac measure at \(t\), and where \(g>0\) and \(a\in \mathbb{R}\).

  2. The Gaussian free field, by choosing \[\mathrm{d}\rho(\varphi_x)=\exp(-a\varphi_x^2)\mathrm{d}\varphi_x\] for a large enough constant \(a\) that depends on \(\beta\).

  3. General \(P(\varphi)\) models, by choosing \[\label{eq:equation32p40phi41} \mathrm{d}\rho(\varphi_x)=\exp(-P(\varphi_x))\mathrm{d}\varphi_x,\tag{1}\] where \(P\) is an even polynomial of degree at least \(4\) and of positive leading coefficient.

For a comprehensive introduction to these models, the interested reader can consult [5][8].

The definition of the model can be extended to include boundary conditions and long-range interactions; see Section 2.1 for the more general definition. We will write \(\nu_{\Lambda, \beta, \rho, J}^{\xi}\) for the finite-volume measure on \(\Lambda\) with inverse temperature \(\beta\), single-site measure \(\rho\), interactions \(J\) and boundary conditions \(\xi\).

Infinite-volume Gibbs measures, defined via the Dobrushin–Lanford–Ruelle (DLR) equation (see Definition 1 below), are objects of central interest in statistical physics, arising naturally as limits of finite-volume measures as \((\Lambda,E)\) tends to an infinite graph such as the lattice \(\mathbb{Z}^d\). Since spins are, in general, unbounded in our setting, this raises the following question: for which boundary conditions is the sequence of measures tight? In the case of the massless Gaussian free field, the Cameron–Martin formula implies that the configuration on \(\Lambda\) under boundary conditions \(\xi\) has the same distribution as the configuration with free boundary conditions on \(\Lambda\) shifted by the harmonic extension of \(\xi\). In particular, if the boundary spins grow to infinity as \(|\Lambda| \rightarrow \infty\), then the sequence is not tight. In contrast, for the massive Gaussian free field, the faster decay of the density of the single-site measure leads to exponential decay of correlations, which in turn allows for tightness of finite-volume measures as long as the boundary conditions grow weakly enough.

Answering this question is more challenging in the non-Gaussian case, for example, when the single-site measure \(\rho\) is such that \[\label{eq:32single-site32n612} \forall a > 0 \quad 0 < \int_{\mathbb{R}} e^{a |u|^{2}} \mathrm{d} \rho(u) < \infty.\tag{2}\] The problem was studied on the lattice \(\mathbb{Z}^{d}\) by Lebowitz and Presutti [1] who proved tightness for boundary conditions that grow like \(\sqrt{\log(\|x\|_{\infty})}\). Their approach utilises a regularity estimate developed by Ruelle [2], [3], which bounds the density at a spin configuration \(\varphi\) in terms of the density at \(\varphi\) of a non-interacting system (i.e.a system with \(\beta = 0\)). See also [9][11] and references therein for related results on infinite-volume Gibbs measures supported on configurations of tempered growth.

The methods of [1] were applied in [4] to the \(\varphi^4\) model on vertex-transitive graphs of polynomial growth. The main result of [4] in this context is that any translation invariant Gibbs measure is a convex combination of two extremal measures, and regularity is needed to construct these extremal measures as limits of finite-volume measures. It was observed in [4] that this result should extend to the setting of vertex-transitive amenable graphs, as previously established for the Ising model [12], but it is not clear how to generalise the regularity estimates of [1] to this case. This provides the motivation for us to develop alternative arguments for proving regularity.

The main result of the present article is a regularity estimate that applies to both nearest-neighbour and long-range interactions on an arbitrary graph. The theorem bounds the Radon–Nikodym derivative of the system in a finite domain \(\Lambda\) at parameter \(\beta>0\), with boundary conditions \(\xi\) that are allowed to grow to infinity as \(|\Lambda|\to\infty\), with respect to a product measure associated with a non-interacting system with a modified single-site measure. The bound is expressed in terms of a function \(A(x,\Lambda,\xi,C)\), where \(x \in \Lambda\) is a vertex and \(C \geq 1\) is a parameter. This function is related to the mean of each spin \(\varphi_x\) and compared to the massless Gaussian free field, it can be interpreted as an analogue of the harmonic extension of \(\xi\). More generally, it plays the role of a non-Gaussian analogue of the Cameron–Martin formula, quantifying the change of measure induced by the boundary conditions. The function \(A(x,\Lambda,\xi,C)\) may take large values when \(x\) is close to the boundary, but it decreases as \(x\) moves further into the bulk, and provided the boundary conditions \(\xi\) do not grow too rapidly, \(A(x,\Lambda,\xi,C)\) remains bounded in the bulk of \(\Lambda\). The formal definition can be found in Section 2.2. For now, let us mention for concreteness that in the case of nearest-neighbour interactions, \[A(x, \Lambda, \xi,C) \approx \max \left\{ 1, \max_{z \in \partial \Lambda} \left(\frac{|\xi_z|}{C}\right)^{(n-1)^{-d(x, z)}} \right\}.\]

We observe a qualitative change in the behaviour of \(A(x,\Lambda,\xi,C)\) depending on the tails of the single-site measure \(\rho\). In order to make this point clearer, let us state the result in the case where \(\rho\) satisfies the stronger assumption \[\label{eq:32single-site32assumption} 0 < \int_{\mathbb{R}} e^{a |u|^{n}} \mathrm{d} \rho(u) < \infty,\tag{3}\] for some \(a>0\) and \(n>2\), a condition satisfied by all the \(P(\varphi)\) models. Here we let \(V\) be a countable set, and we consider interactions \((J_{x, y})_{x, y \in V}\) on \(V\). We call the interactions admissible if they satisfy:

  1. (Symmetry) \(J_{x, y} = J_{y, x}\) for all \(x, y \in V\);

  2. (Integrability) There exists \(f:\mathbb{R} \rightarrow [1, \infty)\) and constants \(\delta_f, M_f > 0\) such that \(f(t) \geq \log(|t|^{-1})^{1/n}\) for all \(t \in (-\delta_f, \delta_f)\), and \(\sum_{y \in V} |J_{x, y}| f(J_{x, y}) \leq M_f\) for all \(x \in V\).

We now state our regularity result, which does not require the interactions \(J\) to be ferromagnetic. Below \(\varphi|_{\Lambda'}\) denotes the restriction of the field to \(\Lambda'\), and \(\mathrm{d} \nu_{\Lambda, \beta, \rho, J}^{\xi}[\varphi|_{\Lambda'} = \psi]\) the density of the restriction.

Theorem 1. Let \(V\) be a countable set and \((J_{x, y})_{x, y \in V}\) be admissible interactions on \(V\). Let \(\beta \geq 0\), \(a > 0\), \(n > 2\) and let \(\rho\) be a single-site measure satisfying 3 . There exist constants \(C \geq 1, \tilde{C} > 0\) such that for any \(\Lambda \subset V\) finite, \(\Lambda' \subset \Lambda\), \(\psi \in \mathbb{R}^{\Lambda'}\), and any boundary conditions \(\xi \in \mathbb{R}^{V}\) with \(\sum_{y \in V} |J_{x, y} \xi_y| < \infty\) for all \(x \in \Lambda\), \[\mathrm{d} \nu_{\Lambda, \beta, \rho, J}^{\xi}[\varphi|_{\Lambda'} = \psi] \leq \left( \prod_{x \in \Lambda'} e^{\tilde{C} A(x, \Lambda, \xi, C)^{n}} \right) \mathrm{d} \nu_{\Lambda', 0, \rho_{\frac{a}{2}}, 0}^{0} [\psi],\] where \(\rho_{\frac{a}{2}}\) is defined by \(\mathrm{d}\rho_{\frac{a}{2}}(u) = e^{\frac{a}{2} |u|^{n}} \mathrm{d} \rho(u)\). Moreover, one can take \(C = C_1 \beta^{\frac{1}{n-2}} + C_2\) and \(\tilde{C} = \tilde{C}_1 \beta^{\frac{n}{n-2}} + \tilde{C}_2\), where \(C_1, C_2, \tilde{C}_1, \tilde{C}_2\) depend only on \(\delta_f,M_f\) and \(\rho\).

Theorem 1 can be generalised to allow for single-site measures that depend on the vertex — see Remark 7 — and to more general Hamiltonians or even conditional measures — see Theorem 8 and Remark 9. We also expect our arguments to be robust enough to apply to models with \(k\)-body interactions, provided 3 is satisfied with \(n > k\), but we do not pursue this here. Furthermore, Theorem 1 applies to arbitrary graphs, thus extending the regularity results of [1] and [4]. In particular, it opens the way for characterising the translation invariant Gibbs measures for the ferromagnetic \(\varphi^4\) model on any vertex-transitive amenable graph, but verifying this is beyond the scope of the current paper.

To illustrate the power of Theorem 1, let us first state a simple but useful application in practice. Below \(\tilde{\rho}\) denotes a vertex-dependent single-site measure defined at vertex \(x \in \Lambda'\) by \(\mathrm{d} \tilde{\rho}_x(u) = \mathbb{1}_{\{u \geq B_x\}} \mathrm{d} \rho_{\frac{a}{2}}(u - B_x)\), where \(B_x\) is a constant which is roughly equal to \(A(x,\Lambda,\xi,C)\). A more precise version of this result can be found in Corollary 3.

Corollary 1. Let \(\Lambda \subset V\) be finite and let \(\xi\) be any boundary conditions such that \(\sum_{y \in V} |J_{x, y} \xi_y|<\infty\) for all \(x \in \Lambda\). Then \(\nu_{\Lambda, \beta, \rho}^{\xi}\) is stochastically dominated by \(\nu_{\Lambda, 0, \tilde{\rho}}^{0}\); hence \(\nu_{\Lambda, \beta, \rho}^{\xi}\) is stochastically dominated by \(\nu_{\Lambda, \beta, \tilde{\rho}}^{0}\).

Remark 2. In contrast to the Cameron–Martin formula for Gaussian fields, our Theorem 1 and Corollary 1 yield only an inequality rather than an exact equality. If \(\xi \geq 0\), one can obtain a reverse inequality by noting that \(\nu_{\Lambda, \beta, \rho}^{\xi}\) stochastically dominates \(\nu_{\Lambda, \beta, \rho}^{0}\), as long as the interactions are ferromagnetic and \(\rho\) is an even measure.

We now outline the proof of Theorem 1, which we believe offers a clearer probabilistic intuition than earlier approaches to regularity. The proof is based on an exploration argument in which we consider the cluster \(\mathcal{C}\) of \(\Lambda'\) consisting of vertices \(x\) for which the spin \(\varphi_x\) takes a large value. To accommodate potentially large boundary conditions, the threshold for including a vertex \(x\) in the cluster is allowed to gradually grow as \(x\) moves further away from \(\Lambda'\), so that it matches the boundary condition \(\xi_z\) at a vertex \(z\) on the boundary of \(\Lambda\). This is where the function \(A(x,\Lambda,\xi,C)\) comes into play; its precise definition enables fine control of the behaviour of \(\mathcal{C}\). In particular, \(A(x,\Lambda,\xi,C)\) is defined so that certain technical conditions relating parents and children in the exploration process are satisfied (see Lemmas 2 and 3). These conditions allow us to isolate each vertex of \(\mathcal{C}\) from its neighbours at a finite cost, thereby yielding a non-interacting system. Finally, we control the size of \(\mathcal{C}\) by comparing it to the total progeny of a subcritical branching process; to carry this out, the parameter \(C\) in the definition of \(A(x,\Lambda,\xi,C)\) must be chosen appropriately. In contrast to [1] and [4], our arguments do not require any assumption of polynomial growth or amenability of the underlying graph.

As an immediate consequence of Theorem 1, we obtain tightness for any boundary conditions such that \(A(x, \Lambda, \xi, C)\) remains bounded for each \(x\in V\) as \(\Lambda \nearrow V\). In the case of ferromagnetic nearest-neighbour interactions, this includes boundary conditions growing like a double exponential of the form \(K^{(n-1)^{d(o, x)}}\), where \(o\) is a fixed origin. This improves on the results of Lebowitz and Presutti [1], which allow only logarithmically growing boundary conditions. In Proposition 10, we show that this result is optimal in the case of non-negative boundary conditions for \(\rho\) defined as in 1 , in the sense that tightness does not occur for non-negative boundary conditions that grow even faster than a constant to the power \((n-1)^{d(o, x)}\). In the case of long-range interactions, the rate of decay of the interactions \(J\) comes into play, as any vertex \(x\) can affect the value of \(\varphi_o\) through the edge \(ox\). This makes characterising the boundary conditions that lead to tightness challenging. Nevertheless, in Proposition 12, we prove that if the interactions \(J\) are well behaved, in the sense that \(|J_{x, y}| \leq d(x, y)^{-r}\) for some \(r > 0\), then we have tightness for boundary conditions growing like \(f(d(o, x)^{-r})\), where \(f\) is a function that encodes the rate of decay of \(J\), i.e.it satisfies [C2] and some additional assumptions.

Coming back to the dependence of the behaviour of \(A(x,\Lambda,\xi,C)\) on the tails of the single-site measure \(\rho\), let us mention that a similar statement (see Theorem 6) to that of Theorem 1 holds if we relax the assumptions on the single-site measure \(\rho\) to allow for any \(\rho\) that satisfies 2 . In this case, we observe a qualitative change in the behaviour of \(A(x, \Lambda, \xi, C)\). For example, in the nearest-neighbour case, we obtain tightness for any boundary conditions growing at most exponentially in the distance, so we observe a jump in the threshold for tightness from exponential to double-exponential at \(n=2\).

Theorems 1 and 6 can be used to obtain regularity for infinite-volume measures, which we define below.

Definition 1. Let \(a>0, \beta \geq 0\), and assume \(J\) satisfies [C1], [C2] and \(\rho\) satisfies 2 . We say that a probability measure \(\nu\) on \(\mathbb{R}^{V}\) with the \(\sigma-\)algebra generated by Borel events depending on finitely many vertices is

  • \(a\)-regular if there exists a constant \(B \in [0, \infty)\) such that for every \(\Lambda \subset V\) finite and \(\psi \in \mathbb{R}^{\Lambda}\), \[\mathrm{d}\nu[\varphi|_{\Lambda} = \psi] \leq e^{B|\Lambda|} \mathrm{d} \nu_{\Lambda, 0, \rho_a, 0}^{0}[\psi],\] where \(\rho_{a}\) is defined by \(\mathrm{d}\rho_{a}(u) = e^{a |u|^{2}} \mathrm{d} \rho(u)\).

  • A Gibbs measure if for every finite \(\Lambda \subset V\) and any bounded measurable function \(g: \mathbb{R}^{\Lambda} \rightarrow \mathbb{R}\), the DLR equation \[\nu[g] = \int_{\xi \in \mathbb{R}^{V}} \langle g\rangle _{\Lambda, \beta, \rho, J}^{\xi} \mathrm{d} \nu(\xi)\] holds. In particular, we assume that \(\nu\) is almost surely supported on configurations \(\xi\) such that \(\langle \cdot \rangle_{\Lambda, \beta, \rho, J}^{\xi}\) is well-defined.

In Section 5.3, we give conditions on \(\xi\) that ensure that the limiting measure (if it exists) as \(\Lambda \nearrow V\) is an \(a\)-regular Gibbs measure. For ferromagnetic interactions, we construct the plus measure \(\nu^{+}\) as the limit of finite-volume measures and show that it is \(a\)-regular for some \(a>0\). We also show that \(\nu^{+}\) is maximal, hence extremal, in the sense that if \(\nu\) is an \(a'\)-regular Gibbs measure for some \(a'>0\), then \(\nu\) is stochastically dominated by \(\nu^{+}\). Furthermore, in the nearest-neighbour case, we introduce a family of finite-volume measures with random boundary conditions that converge to \(\nu^{+}\) and are regular up to the boundary, in contrast to the constructions in [1] and [4], which rely on logarithmically growing boundary conditions. These finite-volume measures are also stochastically decreasing in the volume, similarly to the case of the Ising model. We expect that this may help avoid challenges arising from the absence of maximal boundary conditions at finite volume, leading to simplifications of the arguments in [4] and [13], as well as to applications in future works.

1.1 Paper organisation↩︎

In Section 2, we define the notation that will be used throughout the rest of the paper. Section 3 is dedicated to the proof of Theorem 1. The methods developed here can be applied to a range of other similar models, some examples of which are given in Section 4. In Section 5, we examine for which boundary conditions tightness can be obtained and construct the infinite-volume plus measure as a limit of finite-volume measures.

1.1.0.1 Acknowledgements

We thank Trishen Gunaratnam, Dmitrii Krachun, Romain Panis and Franco Severo for useful discussions. CP was supported by an EPSRC New Investigator Award (UKRI1019).

2 Definitions and preliminaries↩︎

In this section, we define the model in full generality, as well as introduce some additional notation and results that will be used in the proofs.

2.1 Definition of the model↩︎

Let \(V\) be a countably infinite set of vertices. Let \(\beta \geq 0\) be the inverse temperature and let \(\rho\) be a single-site measure satisfying 2 . At some points, including in Theorem 1, we assume \(\rho\) satisfies the stronger condition 3 with respect to some constants \(a >0\) and \(n > 2\). For \(b \in \mathbb{R}\), we will write \(\rho_b\) for the measure with density \(e^{b|u|^{n}}\) with respect to \(\rho\), where we implicitly assume \(n=2\) when we do not require \(\rho\) to satisfy 3 .

Consider interactions \((J_{x, y})_{x, y \in V}\) on \(V\) that satisfy conditions [C1] and [C2]. We will sometimes assume also that the interactions are ferromagnetic, meaning that \(J_{x, y} \geq 0\) for all \(x, y \in V\), but this is not required in our regularity results. Given a finite subset \(\Lambda \subset V\), we denote by \(\overline{E}(\Lambda,J)\) the set of unordered pairs of vertices \(x, y \in V\) with at least one vertex in \(\Lambda\) such that \(J_{x, y} \neq 0\), and write elements of \(\overline{E}(\Lambda,J)\) in the form \(xy\). We define the model on \(\Lambda\) with boundary conditions \(\xi \in \mathbb{R}^{V}\), which we assume satisfy \(\sum_{y \in V} |J_{x, y} \xi_y| < \infty\) for all \(x \in \Lambda\).

Definition 2. The finite-volume spin model on \(\Lambda\) is the measure \(\nu_{\Lambda, \beta, \rho, J}^{\xi}\) on \(\mathbb{R}^{\Lambda}\) given by \[\label{long32range32definition} \mathrm{d} \nu_{\Lambda, \beta, \rho, J}^{\xi}[\varphi] = \frac{1}{Z_{\Lambda, \beta, \rho, J}^{\xi}}\exp(- \beta H_{\Lambda, J}^{\xi}(\varphi)) \prod_{x \in \Lambda} \mathrm{d} \rho(\varphi_x),\qquad{(1)}\] where the partition function \(Z_{\Lambda, \beta, \rho, J}^{\xi}\) is the normalising constant that makes \(\nu_{\Lambda, \beta, \rho, J}^{\xi}\) a probability measure and \(H_{\Lambda, J}^{\xi}(\varphi)\) is the Hamiltonian, given by \[H_{\Lambda, J}^{\xi}(\varphi) = - \sum_{\substack{xy \in \overline{E}(\Lambda, J)\\x, y \in \Lambda}} J_{x, y} \varphi_x \varphi_y - \sum_{\substack{xy \in \overline{E}(\Lambda, J) \\ x \in \Lambda, \, y\in V \setminus \Lambda}} J_{x,y} \varphi_x \xi_y.\]

Let us mention that assumption 2 is necessary for the model to be well-defined for all \(\beta\geq 0\) due to the quadratic nature of the interactions: \[\varphi_x\varphi_y=-\frac{(\varphi_x-\varphi_y)^2}{2}+\frac{\varphi_x^2+\varphi_y^2}{2}.\] We write \(\langle \cdot \rangle_{\Lambda, \beta, \rho, J }^{\xi}\) for the expectation with respect to the measure \(\nu_{\Lambda, \beta, \rho, J}^{\xi}\), and for \(\Lambda' \subset \Lambda\) write \(\nu_{(\Lambda|\Lambda'), \beta, \rho, J}^{\xi}\) for the restriction of \(\nu_{\Lambda, \beta, \rho, J}^{\xi}\) to events that only depend on spins in \(\Lambda'\). For a sequence \((\Lambda_i)_{i \geq 1}\) of finite subsets of \(V\), we say \(\Lambda_i \nearrow V\) if \(\Lambda_i \subset \Lambda_{i+1}\) for all \(i\) and \(\bigcup_{i =1}^{\infty}\Lambda_i = V\). We write \(\Lambda \Subset V\) to denote that \(\Lambda\) is a finite subset of \(V\) and say that the family of measures \((\nu_{\Lambda, \beta, \rho, J}^{\xi})_{\Lambda \Subset V}\) is tight if for any \(\Lambda' \Subset V\), the measures \(\nu_{(\Lambda|\Lambda'), \beta, \rho, J}^{\xi}\) for \(\Lambda' \subset \Lambda \Subset V\) are tight in the usual sense.

The measure \(\nu_{\Lambda, \beta, \rho, J}^{\xi}\) satisfies the domain Markov property, which states that for any \(\Lambda' \subset \Lambda\), \(\psi \in \mathbb{R}^{\Lambda'}, \eta \in \mathbb{R}^{\Lambda \setminus \Lambda'},\) \[\mathrm{d} \nu_{\Lambda, \beta, \rho, J}^{\xi}[\varphi|_{\Lambda'} = \psi \mid \varphi|_{\Lambda \setminus \Lambda'} = \eta] = \mathrm{d} \nu_{\Lambda', \beta, \rho, J}^{\eta \cup \xi}[\psi],\] where \(\eta \cup \xi \in \mathbb{R}^{V}\) is the configuration which is equal to \(\eta\) on \(\Lambda \setminus \Lambda'\) and is equal to \(\xi\) elsewhere.

Another useful property of the model is monotonicity in boundary conditions. Before stating this, we must first introduce the notion of an increasing function.

Definition 3. We say that \(g: \mathbb{R}^{\Lambda} \rightarrow \mathbb{R}\) is an increasing function if for any \(\varphi, \varphi' \in \mathbb{R}^{\Lambda}\) with \(\varphi_x \leq \varphi'_x\) for all \(x \in \Lambda\), then \(g(\varphi) \leq g(\varphi')\). We say an event \(E\) is an increasing event if \(\mathbb{1}_{E}\) is an increasing function. For measures \(\nu, \nu'\) on \(\mathbb{R}^{\Lambda}\), we say that \(\nu\) is stochastically dominated by \(\nu'\) and write \(\nu \preceq \nu'\) if \(\nu[g] \leq \nu'[g]\) for any increasing function \(g: \mathbb{R}^{\Lambda} \rightarrow \mathbb{R}\).

Proposition 3. Suppose \(J\) is ferromagnetic and \(\xi, \xi' \in \mathbb{R}^{V}\) are such that \(\xi_x \leq \xi'_x\) for all \(x \in V\). Then \[\nu_{\Lambda, \beta, \rho, J}^{\xi} \preceq \nu_{\Lambda, \beta, \rho, J}^{\xi'}.\]

Proof. Let \(g: \mathbb{R}^{\Lambda} \rightarrow \mathbb{R}\) be an increasing function, and note that \[F(\varphi) \coloneq \exp(\beta H_{\Lambda, J}^{\xi}(\varphi) - \beta H_{\Lambda, J}^{\xi'}(\varphi)) = \exp\Bigg( \sum_{\substack{xy \in \overline{E}(\Lambda, J) \\ x \in \Lambda, \, y\in V \setminus \Lambda}} \beta J_{x,y} \varphi_x (\xi'_y -\xi_y) \Bigg)\] is an increasing function. Using the FKG inequality [7], we obtain \[\langle g \rangle_{\Lambda, \beta, \rho, J }^{\xi'} = \frac{\langle F g \rangle_{\Lambda, \beta, \rho, J }^{\xi}}{\langle F \rangle_{\Lambda, \beta, \rho, J }^{\xi}} \geq \langle g \rangle_{\Lambda, \beta, \rho, J }^{\xi}.\] ◻

2.2 Definition of \(A(x,\Lambda)\)↩︎

In this section, we introduce the functions \(A(x, \Lambda)\) and \(\tilde{A}(x, \Lambda)\). Before stating the formal definitions, we give the following rough description. Consider a walk from \(x\) to some vertex \(z \in V\) and assign a value to each vertex along the walk, with the value at \(z\) proportional to \(|\xi_z|\). The value at each vertex moving away from \(z\) drops by an amount depending on the interaction strength between the vertices, and we set \(\tilde{A}(x, \Lambda)\) to be the maximum over all walks of the value at \(x\). The function \(A(x, \Lambda)\) is similar, but here we view the boundary conditions \(\xi\) as an external field by combining the contributions from all the vertices in \(V \setminus \Lambda\) that interact with a given vertex \(x \in \Lambda\) into a single point \(h_{x,\Lambda}\), defined as \[h_{x, \Lambda} = \sum_{y \in V \setminus \Lambda} J_{x, y} \xi_y.\] Doing this will ensure that \(A(x, \Lambda)\) is finite for any finite subset \(\Lambda \subset V\), since our assumptions on the boundary conditions \(\xi\) imply that \(|h_{x,\Lambda}| < \infty\) for all \(x \in \Lambda\).

We now give the definitions of \(A(x, \Lambda)\) and \(\tilde{A}(x, \Lambda)\), first stating what we mean by a walk. Let \(R, S, T \subset V\).

  • We say that a sequence of (not necessarily distinct) vertices \(x_0, x_1, \ldots, x_m \in V\) is a walk from \(S\) to \(T\) in \(\overline{(R, J)}\) if \(x_0 \in S, \, x_m \in T\), \(x_1, \ldots, x_{m-1} \in R\), and \(J_{x_{i-1}, x_i} \neq 0\) for all \(i \in \{1, \ldots, m\}\).

  • We say that \(R\) is \(J\)-connected if for any \(x, y \in R\), there exists a walk from \(x\) to \(y\) in \(\overline{(R, J)}\).

When discussing walks to or from a singleton \(\{x\}\), we may write it as \(x\) instead.

We first treat the \(n>2\) case. We give concrete examples in Sections 5.1 and 5.2. For \(n>2\), \(R \subset V\), \(x \in R\) and \(C \geq 1\), define \(\tilde{A}(x,R)=\tilde{A}(x, R, \xi, C, J, f, n)\), to be the smallest \(A \geq 1\) such that for any \(z \in V\) and any walk \(x_0, \ldots, x_m\) from \(x\) to \(z\) in \(\overline{(R, J)}\), \[|\xi_z| \leq C A^{(n-1)^{m}} \prod_{i =1}^{m} f(J_{x_{i-1}, x_{i}})^{(n-1)^{m-i}}.\] if such \(A\) exists, and otherwise we say that \(\tilde{A}(x, R) = \infty\). Note that \(\tilde{A}(x, R)\) is increasing in \(R\). We also define \(A(x,R)=A(x, R, \xi, C, J, f, n)\) to be the smallest \(A \geq 1\) such that for any \(y \in R\) and any walk \(x_0, x_1,\ldots, x_{m}\) from \(x\) to \(y\) in \(\overline{(R, J)}\), \[|h_{y, R}| \leq \left( \sum_{z \in V \setminus R} |J_{y, z}| f(J_{y,z}) \right) C A^{(n-1)^{m+1}} \prod_{i =1}^{m} f(J_{x_{i-1}, x_{i}})^{(n-1)^{m+1-i}},\] and say that \(A(x, R) = \infty\) if no such \(A\) exists.

We now give the definition in the \(n=2\) case. For \(R \subset V\), \(x \in R\), \(C\geq 1\) and \(\lambda \geq 1\), we define \(\tilde{A}(x, R) = \tilde{A}(x, R, \lambda, \xi, C, J, f)\) to be the smallest \(A\geq 1\) such that for any \(z \in V\) and any walk \(x_0, x_1, \ldots, x_m\) from \(x\) to \(z\) in \(\overline{(R, J)}\), \[|\xi_z| \leq C A \lambda^{m} \prod_{i=1}^{m} f(J_{x_{i-1}, x_i}).\] We also define \(A(x, R) = A(x, R, \lambda, \xi, C, J, f)\) to be the smallest \(A\geq 1\) such that for any walk \(x_0, x_1, \ldots, x_m\) from \(x\) to \(R\) in \(\overline{(R, J)}\), \[|h_{x_m, R}| \leq \left(\sum_{z \in V \setminus R} |J_{x_m, z}| f(J_{x_m, z}) \right) C A \lambda^{m+1} \prod_{i=1}^{m} f(J_{x_{i-1}, x_i}).\]

We will frequently drop the parameters \(\xi, C, J, f, n, \lambda\) from the notation when they are clear from the context. In both cases \(n>2\) and \(n=2\), it follows (from Theorem 1 and Theorem 6 respectively) that we have tightness if \(A(x, \Lambda)\) is bounded above by a function of \(x\) that does not depend on \(\Lambda\). When considering whether this is the case for a particular choice of boundary conditions, it may be more convenient to work with the function \(\tilde{A}\) and use the fact that for any \(\Lambda \Subset V\) and any \(x \in \Lambda\) we have \(A(x, \Lambda) \leq \tilde{A}(x, \Lambda) \leq \tilde{A}(x, V)\). To see why this is the case, let \(y \in \Lambda\) and let \(x_0, \ldots, x_m\) be a walk from \(x\) to \(y\) in \(\overline{(\Lambda, J)}\). Suppose \(n>2\) (the \(n=2\) case is similar). For any \(z \in V\) with \(J_{y,z} \neq 0\), the definition of \(\tilde{A}(x, \Lambda)\) applied to the walk \(x_0, \ldots, x_m, z\) implies that \[|\xi_z| \leq C \tilde{A}(x, \Lambda)^{(n-1)^{m+1}} f(J_{y,z}) \prod_{i =1}^{m} f(J_{x_{i-1}, x_{i}})^{(n-1)^{m+1-i}},\] hence \[\begin{align} |h_{y, \Lambda}| &\leq \sum_{z \in V \setminus \Lambda} |J_{y, z}| |\xi_z|\\ &\leq \left( \sum_{z \in V \setminus \Lambda} |J_{y, z}| f(J_{y,z}) \right) C \tilde{A}(x, \Lambda)^{(n-1)^{m+1}} \prod_{i =1}^{m} f(J_{x_{i-1}, x_{i}})^{(n-1)^{m+1-i}}, \end{align}\] which implies \(A(x, \Lambda) \leq \tilde{A}(x, \Lambda)\). Since \(\tilde{A}(x, R)\) is increasing in \(R\), we obtain tightness if \(\tilde{A}(x, V)\) is finite for all \(x \in V\). For \(n>2\), define \(\Xi = \Xi(V, J, f, n)\) to be the set of boundary conditions for which this is the case. Similarly, for \(n=2\), define \(\Xi(\lambda)\) to be the set of boundary conditions for which \(\tilde{A}(x, V,\lambda)\) is finite for all \(x \in V\). See Sections 5.1 and 5.2 for examples of boundary conditions that are in \(\Xi\) for different choices of interactions \(J\).

We now state a lemma that allows us to compare the values of \(A(x, R)\) and \(A(y, R)\) or \(\tilde{A}(x, R)\) and \(\tilde{A}(y, R)\). In the case when \(V\) is \(J\)-connected, this means that to determine whether given boundary conditions are in \(\Xi\), it suffices to check whether \(\tilde{A}(x, V)\) is finite for one vertex \(x\).

Lemma 1. Let \(R \subset V\), \(C \geq 1\), and \(\xi \in \mathbb{R}^{V}\). For any walk \(x_0, x_1, \ldots, x_k\) in \(\overline{(R, J)}\) with \(x_0, x_k \in R\), we have \[\begin{align} &\text{(i) If } n > 2, \quad \tilde{A}(x_k, R) \leq \tilde{A}(x_0, R)^{(n-1)^{k}} \prod_{i=1}^{k} f(J_{x_{i-1}, x_i})^{(n-1)^{k-i}},\\ &\text{(ii) If } n > 2, \quad A(x_k, R) \leq A(x_0, R)^{(n-1)^{k}} \prod_{i=1}^{k} f(J_{x_{i-1}, x_i})^{(n-1)^{k-i}},\\ &\text{(iii) If n=2, \quad \tilde{A}(x_k, R) \leq \tilde{A}(x_0, R) \lambda^{k} \prod_{i=1}^{k} f(J_{x_{i-1}, x_i})},\\ &\text{(iv) If n=2, \quad A(x_k, R) \leq A(x_0, R) \lambda^{k} \prod_{i=1}^{k} f(J_{x_{i-1}, x_i})}. \end{align}\]

Proof. The proofs of the first two and last two statements are very similar, so we only prove (i) and (iv) here. For (i), let \(z \in V\) and let \(y_0, y_1, \ldots, y_j\) be a walk from \(x_k\) to \(z\) in \(\overline{(R, J)}\). Considering the walk \(x_0, \ldots, x_k, y_1, \ldots, y_j\), then by definition of \(\tilde{A}(x_{0}, R)\), we have \[|\xi_{z}| \leq C \tilde{A}(x_0, R)^{(n-1)^{k+j}} \left(\prod_{i = 1}^{k} f(J_{x_{i-1}, x_i})^{(n-1)^{k+j-i}} \right) \left(\prod_{i = 1}^{j} f(J_{y_{i-1}, y_i})^{(n-1)^{j-i}} \right).\] Hence \(\tilde{A}(x_0, R)^{(n-1)^{k+j}} \prod_{i = 1}^{k} f(J_{x_{i-1}, x_i})^{(n-1)^{k+j-i}}\) satisfies the requirements for \(\tilde{A}(x_k, R)^{(n-1)^{j}}\), so \[\begin{align} \tilde{A}(x_k, R)^{(n-1)^{j}} &\leq \tilde{A}(x_0, R)^{(n-1)^{k+j}} \left(\prod_{i = 1}^{k} f(J_{x_{i-1}, x_i})^{(n-1)^{k+j-i}} \right)\\ &= \left( \tilde{A}(x_0, R)^{(n-1)^{k}} \prod_{i = 1}^{k} f(J_{x_{i-1}, x_i})^{(n-1)^{k-i}} \right)^{(n-1)^j}. \end{align}\] Taking both sides to the power \(1/(n-1)^j\) yields (i).

To prove (iv), let \(y \in R\) and let \(y_0, y_1, \ldots, y_j\) be a walk from \(x_k\) to \(y\) in \(\overline{(R, J)}\). Considering the walk \(x_0, \ldots, x_k, y_1, \ldots, y_j\), then by definition of \(A(x_{0}, R)\), we have \[|h_{y, R}| \leq \left(\sum_{z \in V \setminus R} |J_{y, z}| f(J_{y, z}) \right) C A(x_0,R) \lambda^{k+j+1} \prod_{i=1}^{k} f(J_{x_{i-1}, x_i})\prod_{i=1}^j f(J_{y_{i-1}, y_i}).\] This means that \(A(x_0,R)\lambda^{k} \prod_{i=1}^{k} f(J_{x_{i-1}, x_i})\) satisfies the requirements for \(A(x_k,R)\), which yields (iv). ◻

2.3 Branching processes↩︎

In the proof of our main regularity theorem, we will use a standard result on branching processes from [14] to bound the size of the cluster where the spins take large values. Below we give the definition of a branching process and then state this result.

For a random variable \(X\) taking values in the non-negative integers, a branching process with offspring distribution \(X\) and initial population \(k \in \mathbb{N}\) is a sequence of random variables \((Z_n)_{n \geq 0}\) such that \(Z_0 = k\) and for all \(n \geq 1\), \(Z_n = \sum_{i=1}^{Z_{n-1}} X_{n, i}\), where \(X_{n, i}\) are independent random variables with the same distribution as \(X\). We call \(T:=\sum_{n=0}^{\infty} Z_n\) the total progeny of the branching process.

Theorem 4 (). For a branching process with offspring distribution \(X\) and initial population \(k\), the distribution of the total progeny \(T\) is given by \[\mathbb{P}[T = n] = \frac{k}{n} \mathbb{P}[X_1 + \ldots + X_n = n-k],\] where \(X_1, \ldots, X_n\) are independent random variables with the same distribution as \(X\).

3 Proof of Theorem 1↩︎

In this section, we prove Theorem 1 by employing an exploration argument. We start by gathering some useful inequalities.

Lemma 2. Let \(\beta>0\), \(n\geq 2\), \(\alpha_0\geq 1\) and \(C\geq \alpha_0\). For every \(x, y \in V\), \(|\varphi_x|\geq C\), and \(t_x, t_y \in [-\alpha_0, \alpha_0]\), \[\beta (|\varphi_x| |\varphi_y| + |t_x||t_y|) \leq \frac{2\beta}{C^{n-2}}(|\varphi_x|^{n}+|\varphi_y|^{n} ).\]

Proof. By Young’s inequality and the fact that \(|t_x|,|t_y|\leq |\varphi_x|\), \[\label{eq:Young32inequality} \beta (|\varphi_x| |\varphi_y| + |t_x||t_y|) \leq \frac{\beta}{2} (|\varphi_x|^{2} + |\varphi_y|^{2}+|t_x|^2+|t_y|^2)\leq \frac{\beta}{2}(3|\varphi_x|^{2}+|\varphi_y|^{2}).\tag{4}\] If \(|\varphi_y|<C\), then 4 implies that \[\beta (|\varphi_x| |\varphi_y| + |t_x||t_y|) \leq 2\beta |\varphi_x|^2\leq \frac{2\beta}{C^{n-2}}|\varphi_x|^n.\] If \(|\varphi_y|\geq C\), then 4 gives \[\beta (|\varphi_x| |\varphi_y| + |t_x||t_y|) \leq \frac{\beta}{2C^{n-2}}(3|\varphi_x|^{n}+|\varphi_y|^{n})\leq \frac{3\beta}{2C^{n-2}}(|\varphi_x|^{n}+|\varphi_y|^{n}).\] This completes the proof. ◻

Lemma 3. Let \(\beta, a>0\), \(n>2\), \(\alpha_0\geq 1\) and \(C\geq \alpha_0+\left(\frac{4M_f\beta}{a}\right)^{\frac{1}{n-2}}\). If \(|\varphi_x| \geq C\) and \(|\varphi_y| \leq \frac{f(J_{x,y})}{C^{n-2}}|\varphi_x|^{n-1}\), then for any \(t \in [-\alpha_0, \alpha_0]\), \[\beta (|\varphi_x| |\varphi_y| + |t||\varphi_y|) \leq \frac{a f(J_{x, y})}{2 M_f} |\varphi_x|^{n}.\]

Proof. Note that since \(|\varphi_y| \leq \frac{f(J_{x,y})}{C^{n-2}}|\varphi_x|^{n-1}\), we have \[\begin{align} \beta |\varphi_y| (|\varphi_x| + |t|) -\frac{a f(J_{x, y})}{2M_{f}} |\varphi_x|^{n} &\leq \beta f(J_{x, y}) \frac{|\varphi_x|^{n-1}}{C^{n-2}} (|\varphi_x| + |t|)-\frac{a f(J_{x, y})}{2 M_{f}} |\varphi_x|^{n}\\ &\leq f(J_{x, y}) |\varphi_x|^{n} \left( \frac{\beta}{C^{n-2}} \left(1 + \frac{\alpha_0}{|\varphi_x|}\right) - \frac{a}{2M_f} \right). \end{align}\] For every \(C\geq \alpha_0 + (4a^{-1}M_f\beta)^\frac{1}{n-2}\), the above expression is negative when \(|\varphi_x| \geq C\). ◻

We now proceed with the proof of Theorem 1. Recall that we consider \(\Lambda'\subset \Lambda\). Our approach is based on an exploration process that builds the cluster \(\mathcal{C}\) of vertices \(x\) such that there exists a walk from \(\Lambda'\) to \(x\) where the spins take large values at each vertex along the walk. To accommodate the potentially large boundary conditions, we allow the minimum spin value needed to be in \(\mathcal{C}\) to grow progressively as we move away from \(\Lambda'\), ensuring that no vertices in \(V \setminus \Lambda\) are included in \(\mathcal{C}\). This gradual growth ensures that the conditions of Lemmas 2 and 3 are satisfied, which in turn enables us to isolate the vertices of \(\mathcal{C}\) from their neighbours, at the cost of modifying the single-site measure. For those vertices in \(\Lambda'\) where the spins take small values, we estimate their contribution to the Radon–Nikodym derivative directly.

Proof of Theorem 1. Fix a finite subset \(\Lambda \subset V\) and let \(\Lambda' \subset \Lambda\). We write \(E\) for \(\{xy \in \overline{E}(\Lambda, J): x,y \in \Lambda\}\) and \(A_x\) for \(A(x, \Lambda, \xi, C, J, f, n)\), where \(C \geq 1\) is a constant to be determined. Define \(\mathcal{C}\) to be the set of vertices \(x \in \Lambda\) such that for some \(m \in \{ 0, 1, \ldots\}\) there exists a walk \(x_0, x_1, \ldots, x_m\) from \(\Lambda'\) to \(x\) in \(\overline{(\Lambda, J)}\) that satisfies \[\label{cluster32membership32criteria} \forall k \in S_m \quad |\varphi_{x_k}| \geq C A_{x_0}^{(n-1)^{k}} \prod_{i = 1}^{k} f(J_{x_{i-1}, x_i})^{(n-1)^{k-i}},\tag{5}\] where \(S_0 = \{0\}\) and \(S_m = \{1, \ldots, m\}\) for \(m \geq 1\). For each \(i \in \{ 0, 1, \ldots\}\), let \(\mathcal{C}_i\subset \mathcal{C}\) denote the set of vertices for which \(i\) is the smallest value of \(m\) such that there exists a walk satisfying 5 . Note that if \(x \in \mathcal{C}\), then \(|\varphi_x| \geq C\), and if \(y \in \Lambda'\), then Lemma 1 implies that \(y\in \mathcal{C}\) if and only if \(y \in \mathcal{C}_0\), that is, if and only if \(|\varphi_y| \geq CA_y\).

Our aim is to prove that there exists \(K \geq 0\) such that for any \(V_1, V_2, \ldots\) pairwise disjoint subsets of \(\Lambda \setminus \Lambda'\) we have \[\begin{align} \label{eq:branching32process32comparison} &\mathrm{d}\nu_{\Lambda, \beta, \rho, J}^{\xi} \left[ \varphi|_{\Lambda'}, \, (\mathcal{C}_i)_{i \geq 1} = (V_i)_{i \geq 1} \right] \leq \\ \nonumber &\exp \left(K|\Lambda'\cup V'| \right) \left( \prod_{x \in \Lambda'} e^{\alpha_1 M_f A_{x}^{n}} \mathrm{d} \rho_{\frac{a}{2}}(\varphi_x) \right) \prod_{i = 0}^{\infty} \prod_{y \in V_{i+1}} \max_{x \in V_i} p_{x, y}, \end{align}\tag{6}\] where \(\alpha_1=2\beta C^2\), \(V_0 = \Lambda'\), \(V' = \bigcup_{i = 1}^{\infty} V_i\), and \[p_{x, y} = \begin{cases} \int_{|u| \geq C f(J_{x,y})} \mathrm{d} \rho_{\frac{a}{2}}(u) & \text{if } J_{x,y} \neq 0, \\ 0 & \text{if } J_{x,y} = 0. \end{cases}\] Here \((p_{x, y})_{x, y \in V}\) can be interpreted as the offspring distribution of a branching process in the sense that \(y\) is a child of \(x\) with probability \(p_{x, y}\). The distribution of the number of children of vertex \(x\) in this process depends on \(x\), but we can get a uniform control of the distribution by tuning the value of \(C\).

Assume that 6 holds for now. Summing 6 over all possibilities \((V_j)\) for \((\mathcal{C}_j)\) and noting that \(\Lambda' \cap V' = \emptyset\) on the event \(\{(\mathcal{C}_i)_{i \geq 1} = (V_i)_{i \geq 1}\}\), we obtain \[\begin{align} \mathrm{d}\nu_{\Lambda, \beta, \rho, J}^{\xi} \left[ \varphi|_{\Lambda'}\right] \leq \nonumber \left( \prod_{x \in \Lambda'} e^{\alpha_1 M_f A_{x}^{n}} \mathrm{d} \rho_{\frac{a}{2}}(\varphi_x) \right) \sum_{(V_j)} e^{K(|\Lambda'|+|V'|)}\prod_{i = 0}^{\infty} \prod_{y \in V_{i+1}} \max_{x \in V_i} p_{x, y}. \end{align}\] We can thus conclude by applying Lemma 5, which bounds the right-hand side.

Let us now prove 6 . Let \(\alpha_0 \geq 1\) be such that \(\rho_{a}([-\alpha_0, \alpha_0]) > 0\). Given \((\mathcal{C}_i)_{i \geq 1} = (V_i)_{i \geq 1}\) with \(\bigcup_{i = 1}^{\infty} V_i = V'\), let \(t \in [-\alpha_0, \alpha_0]^{\Lambda' \cup V'}\) and define \(\tilde{\varphi} \in \mathbb{R}^{\Lambda}\) to be the configuration with \(\tilde{\varphi}_x = t_x\) for \(x \in \Lambda' \cup V'\) and \(\tilde{\varphi_x} = \varphi_x\) for \(x \in \Lambda \setminus (\Lambda' \cup V')\). Comparing the value of the integrand at \(\varphi\) with its value at \(\tilde{\varphi}\) and setting \(\alpha_1 = 2 \beta C^{2}\), we will see that we can choose \(C\) large enough that \[\begin{align} \label{compactified32inequality} &\beta J_{x,y} \varphi_x \varphi_y \leq \beta J_{x,y} \tilde{\varphi}_x \tilde{\varphi}_y\\ \nonumber & + |J_{x,y}| f(J_{x, y}) \left(\frac{a|\varphi_x|^{n}}{2M_f}\mathbb{1}_{x\in \mathcal{C}}+\alpha_1 A_x^n\mathbb{1}_{x\in \Lambda' \setminus \mathcal{C}}+\frac{a|\varphi_y|^{n}}{2M_f}\mathbb{1}_{y\in \mathcal{C}}+\alpha_1 A_y^n \mathbb{1}_{y\in \Lambda' \setminus \mathcal{C}} \right). \end{align}\tag{7}\] We now verify 7 by considering an edge \(xy \in E\) and splitting into cases based on whether \(x\) and \(y\) are in \(\mathcal{C}\), \(\Lambda' \setminus \mathcal{C}\), or \(\Lambda \setminus (\Lambda' \cup \mathcal{C})\). In each case we will use the bound \(\beta J_{x,y}(\varphi_x \varphi_y - \tilde{\varphi}_x \tilde{\varphi}_y) \leq \beta |J_{x,y}| (|\varphi_x| |\varphi_y| + |\tilde{\varphi}_x| |\tilde{\varphi}_y|)\).

  • If \(x, y \in \mathcal{C}\), then \(|\varphi_x|, |\varphi_y| \geq C\), so by Lemma 2, if \(C\geq \alpha_0+\left(\frac{4M_f\beta}{a}\right)^{\frac{1}{n-2}}\), then \[\beta (|\varphi_x| |\varphi_y| + |t_x||t_y|) \leq \frac{a f(J_{x, y})}{2 M_f} ( |\varphi_x|^{n} + |\varphi_y|^{n}).\]

  • If \(x \in \mathcal{C}\) and \(y \in \Lambda \setminus (\Lambda' \cup \mathcal{C})\), then there exists a walk \(x_0, x_1, \ldots, x_m\) from \(\Lambda'\) to \(x\) in \(\overline{(\Lambda, J)}\) satisfying 5 , but there is no such walk from \(\Lambda'\) to \(y\). Hence the walk \(x_0, \ldots, x_m, y\) does not satisfy 5 , so \[\begin{align} |\varphi_y| &\leq C A_{x_0}^{(n-1)^{m+1}} f(J_{x, y}) \prod_{i = 1}^{m} f(J_{x_{i-1}, x_i})^{(n-1)^{m+1-i}}\\ &= \frac{f(J_{x, y})}{C^{n-2}} \left(C A_{x_0}^{(n-1)^{m}} \prod_{i = 1}^{m} f(J_{x_{i-1}, x_i})^{(n-1)^{m-i}} \right)^{n-1} \leq \frac{f(J_{x, y})}{C^{n-2}} |\varphi_x|^{n-1}. \end{align}\] Combining the latter with Lemma 3 we get \[\beta (|\varphi_x| |\varphi_y| + |t_x||\varphi_y|) \leq \frac{a f(J_{x, y})}{2 M_f} |\varphi_x|^{n}.\]

  • If \(x \in \mathcal{C}\) and \(y \in \Lambda' \setminus \mathcal{C}\), then applying Lemma 2 with \(C \geq \alpha_0+\left(\frac{4M_f\beta}{a}\right)^{\frac{1}{n-2}}\) and using that \(|\varphi_y|\leq CA_y\), we get \[\begin{align} \beta (|\varphi_x| |\varphi_y| + |t_x| |t_y|) &\leq \frac{2\beta}{C^{n-2}}(|\varphi_x|^{n}+(CA_y)^n) \leq \frac{a f(J_{x, y})}{2 M_f}|\varphi_x|^{n} + 2\beta C^{2} A_{y}^{n}. \end{align}\]

  • If \(x, y \in \Lambda' \setminus \mathcal{C}\), then \(|\varphi_x| \leq CA_x\) and \(|\varphi_y| \leq CA_y \leq CA_{x}^{n-1}f(J_{x, y})\) by Lemma 1, so \[\beta (|\varphi_x| |\varphi_y| + |t_x| |t_y|) \leq 2 \beta C^{2} A_x^n f(J_{x,y}).\]

  • If \(x \in \Lambda' \setminus \mathcal{C}\) and \(y \in \Lambda \setminus (\Lambda' \cup \mathcal{C})\), then \(|\varphi_x| \leq CA_x\) and \(|\varphi_y| \leq CA_{x}^{n-1}f(J_{x, y})\), so \[\begin{align} \beta (|\varphi_x| |\varphi_y| + |t_x||\varphi_y|) \leq 2 \beta C^{2} A_x^n f(J_{x,y}). \end{align}\]

The terms \(e^{\beta h_{x,\Lambda} \varphi_x}\) coming from interaction with the spins outside \(\Lambda\) can be bounded similarly, using that if \(x \in \mathcal{C}\), then by definition of \(\mathcal{C}\) and \(A_x\) we have \[|h_{x, \Lambda}| \leq \left(\sum_{y \in V \setminus \Lambda} |J_{x, y}| f(J_{x,y}) \right) \frac{|\varphi_x|^{n-1}}{C^{n-2}},\] so Lemma 3 applies. If \(x \in \Lambda' \setminus \mathcal{C}\) then we bound \(|h_{x, \Lambda}|\) using the definition of \(A_x\). Overall, we obtain \[\label{compactified32inequality322} \beta h_{x,\Lambda} \varphi_x \leq \beta h_{x, \Lambda} \tilde{\varphi}_x + \left( \frac{a|\varphi_x|^{n}}{2M_f}\mathbb{1}_{x\in \mathcal{C}}+\alpha_1 A_x^n\mathbb{1}_{x\in \Lambda' \setminus \mathcal{C}} \right) \sum_{y \in V \setminus \Lambda} |J_{x, y}| f(J_{x,y}).\tag{8}\]

Now 6 follows from Lemma 4 below, which we also state in the case \(n=2\). It only remains to show that we can choose \(C\) and \(\tilde{C}\) of the required form. Note that \(C\) depends on \(\beta\) only through the condition \(C\geq \alpha_0+\left(\frac{4M_f\beta}{a}\right)^{\frac{1}{n-2}}\) when applying Lemmas 2 and 3. We can choose \(\tilde{C} = \log(\alpha_2 \int_{\mathbb{R}} \mathrm{d} \rho_{\frac{a}{2}}(u)) + \alpha_1 M_f\), where \(\alpha_2\) is given by Lemma 5 and does not depend on \(\beta\). Hence the only dependence of \(\tilde{C}\) on \(\beta\) comes from \(\alpha_1 = 2 \beta C^{2}\). ◻

Lemma 4. Assume that [C1], [C2], 7 and 8 hold for some \(n\geq 2\), \(a>0,\alpha_1>0\) and \(A_x\geq 1\), where \(\tilde{\varphi}\) in 7 and 8 is defined as above for \(\alpha_0 \geq 1\) such that \(\rho_{a}([-\alpha_0, \alpha_0]) > 0\). Then there exists a constant \(K=K(a,\alpha_0) \geq 0\) such that \[\begin{align} &\mathrm{d}\nu_{\Lambda, \beta, \rho, J}^{\xi} \left[ \varphi|_{\Lambda'}, \, (\mathcal{C}_i)_{i \geq 1} = (V_i)_{i \geq 1} \right] \leq \\ \nonumber &\exp \left(K|\Lambda'\cup V'| \right) \left( \prod_{x \in \Lambda'} e^{\alpha_1 M_f A_{x}^{n}} \mathrm{d} \rho_{\frac{a}{2}}(\varphi_x) \right) \prod_{i = 0}^{\infty} \prod_{y \in V_{i+1}} \max_{x \in V_i} p_{x, y}. \end{align}\]

Proof. For ease of notation, write \(P_{\Lambda}(\varphi) = \prod_{x \in \Lambda} e^{-a|\varphi_x|^{n}}\) and \[\pi_{E}(\varphi) = \left(\prod_{xy \in E} e^{\beta J_{x, y} \varphi_x \varphi_y} \right) \left( \prod_{x \in \Lambda} e^{\beta h_{x, \Lambda} \varphi_x}\right).\] Note that ?? gives that \[\begin{align} &\mathrm{d} \nu_{\Lambda, \beta, \rho, J}^{\xi} \left[ \varphi|_{\Lambda'}, \, (\mathcal{C}_i)_{i \geq 1} = (V_i)_{i \geq 1} \right] = \frac{1}{Z_{\Lambda, \beta, \rho, J}^{\xi}} \int_{\mathbb{R}^{\Lambda \setminus \Lambda'}} \mathbb{1}_{\{(\mathcal{C}_i)_{i \geq 1} = (V_i)_{i \geq 1}\}} \pi_{E}(\varphi) P_{\Lambda}(\varphi) \prod_{x \in \Lambda} \mathrm{d} \rho_{a}(\varphi_x), \end{align}\] where \(\rho_a\) satisfies \(0 < \rho_{a}(\mathbb{R})<\infty\). We estimate \(\pi_{E}(\varphi)\) by applying 7 to each element of the first product and 8 to each element of the second product. This yields \[\pi_{E}(\varphi) \leq \prod_{x \in \Lambda' \setminus \mathcal{C}} \exp \left( \alpha_1 A_{x}^{n} \sum_{y \in V} |J_{x, y}| f(J_{x, y}) \right) \prod_{x \in \mathcal{C}} \exp \left( \frac{a|\varphi_x|^{n}}{2 M_f} \sum_{y \in V} |J_{x, y}| f(J_{x, y})\right) \pi_{E}(\tilde{\varphi}).\] Using [C2] the above inequality simplifies to \[\begin{align} \pi_{E}(\varphi) &\leq \left( \prod_{x \in \Lambda'} e^{\alpha_1 M_f A_{x}^{n}} \right) \left(\prod_{x \in \mathcal{C}} e^{\frac{a}{2}|\varphi_x|^{n}}\right) \pi_{E}(\tilde{\varphi}). \end{align}\] Combining this with the product over vertices of the terms coming from the single-site measure, and using that \(|t_x| \leq \alpha_0\) for any \(x \in \Lambda' \cup V'\), we get \[\begin{align} \label{eq:pi32P32inequality} \pi_{E}(\varphi) P_{\Lambda}(\varphi) &\leq \left( \prod_{x \in \Lambda'} e^{\alpha_1 M_f A_{x}^{n}} \right) \left( \prod_{x \in \Lambda'\cup V'} e^{-\frac{a}{2}|\varphi_x|^{n}} \right) \pi_{E}(\tilde{\varphi}) P_{\Lambda \setminus (\Lambda' \cup V')}(\tilde{\varphi})\\ &\leq \exp \left(a \alpha_{0}^{n} |\Lambda'\cup V'| \right) \left( \prod_{x \in \Lambda'} e^{\alpha_1 M_f A_{x}^{n}} \right) \left( \prod_{x \in \Lambda'\cup V'} e^{-\frac{a}{2}|\varphi_x|^{n}} \right) \pi_{E}(\tilde{\varphi}) P_{\Lambda}(\tilde{\varphi}) \notag. \end{align}\tag{9}\] We now integrate with respect to \(\varphi_x\) for each \(x \in \Lambda \setminus \Lambda'\) over the event \(\{(\mathcal{C}_i)_{i \geq 1} = (V_i)_{i \geq 1}\}\). Observe that, on this event, if \(y \in V_{i + 1}\) for some \(i \in \{0, 1, \ldots\}\), then \(|\varphi_y| \geq C f(J_{x, y})\) for some \(x \in V_i\) with \(J_{x, y} \neq 0\). Hence, ignoring the requirement for spins outside \(\mathcal{C}\) to be small, we have \[\label{eq:32integral32p32bound} \int_{\mathbb{R}^{V'}} \mathbb{1}_{\{(\mathcal{C}_i)_{i \geq 1} = (V_i)_{i \geq 1}\}} \prod_{x \in V'} e^{-\frac{a}{2}|\varphi_x|^{n}} \mathrm{d} \rho_{a}(\varphi_x) \leq \prod_{i = 0}^{\infty} \prod_{y \in V_{i+1}} \max_{x \in V_i} p_{x, y}.\tag{10}\] Note that for any function \(F: \mathbb{R}^{\Lambda' \cup V'} \to \mathbb{R}_{\geq 0}\), \[\begin{align} \nonumber \rho_{a}([-\alpha_0, \alpha_0])^{|\Lambda' \cup V'|}\min_{t \in [-\alpha_0, \alpha_0]^{\Lambda' \cup V'}} F(t) &\leq \int_{[-\alpha_0, \alpha_0]^{\Lambda' \cup V'}} F(t) \prod_{x \in \Lambda' \cup V'}\mathrm{d} \rho_{a}(t_x)\\ \label{eq:min} &\leq \int_{\mathbb{R}^{\Lambda' \cup V'}}F(t) \prod_{x \in \Lambda' \cup V'}\mathrm{d} \rho_{a}(t_x). \end{align}\tag{11}\] Thus, since \(t \in [-\alpha_0, \alpha_0]^{\Lambda' \cup V'}\) is arbitrary in the definition of \(\tilde{\varphi}\), integrating 9 and dividing by \(Z_{\Lambda, \beta, \rho, J}^{\xi}\), applying 11 for \(F\) being \(\pi_{E}(\tilde{\varphi}) P_{\Lambda}(\tilde{\varphi})\), and using 10 yields 6 , with \(K = \max \{0, a \alpha_{0}^{n} - \log(\rho_{a}([-\alpha_0, \alpha_0]))\}\). ◻

We now state and prove the second lemma used in the proof of Theorem 1 above, which we also state in the case \(n=2\). We use the same notation as in the proof of Theorem 1, and we recall that the definition of \(p_{x,y}\) involves a constant \(C\).

Lemma 5. Let \(n\geq 2\) and \(K\geq0\). Then there exist \(C_0,\alpha_2\geq 1\) that do not depend on \(\beta\) such that for every \(C\geq C_0\) we have \[\sum_{(V_j)} e^{K(|\Lambda'|+|V'|)}\prod_{i = 0}^{\infty} \prod_{y \in V_{i+1}} \max_{x \in V_i} p_{x, y}\leq \alpha_2^{|\Lambda'|}.\]

Proof. We aim to compare \(\prod_{i = 0}^{\infty} \prod_{y \in V_{i+1}} \max_{x \in V_i} p_{x, y}\) with the probability that \(W_i = V_i\) for all \(i \geq 1\), where \((W_{i})_{i \geq 0}\) is the exploration process defined as follows. First set \(W_0 = \Lambda'\) and ensure that \(C\) is chosen large enough that \(\int_{|u| \geq C} \mathrm{d} \rho_{\frac{a}{2}}(u) \leq 1\). Assuming that \(W_i\) has already been constructed, for each vertex \(x \in W_i\) and \(y \in \Lambda \setminus (W_0 \cup \ldots \cup W_i)\), say that the edge \(xy\) is open with probability \(p_{x, y}\), independently of all other edges. Otherwise, say \(xy\) is closed. Then set \(W_{i+1}\) to be the set of vertices \(y \in \Lambda \setminus (W_0 \cup \ldots \cup W_i)\) such that \(xy\) is open for some \(x \in W_i\). Once \(W_i\) has been constructed for all \(i \in \{0, 1, \ldots \}\), set \(W = \bigcup_{i=1}^{\infty} W_i\). With this definition, we have \[\begin{align} &\mathbb{P}[W_{i+1} = V_{i+1} | W_1 = V_1, \ldots, W_i = V_i] =\\ &\prod_{y \in \Lambda \setminus (V_0 \cup \ldots \cup V_{i+1})} \mathbb{P} \left[ \bigcap_{x \in V_i} \{ xy \text{ closed} \}\right] \prod_{y \in V_{i+1}} \mathbb{P} \left[ \bigcup_{x \in V_i} \{ xy \text{ open} \}\right] \geq b^{|V_i|} \prod_{y \in V_{i+1}} \max_{x \in V_i} p_{x, y}, \end{align}\] where \[b = \inf_{x \in V} \prod_{y \in V \setminus \{x\}} (1-p_{x, y}).\] Combining over all generations of the exploration process, we obtain \[\begin{align} \nonumber \mathbb{P}[(W_{i})_{i \geq 1} = (V_i)_{i \geq 1}] &= \prod_{i = 0}^{\infty} \mathbb{P}[W_{i+1} = V_{i+1} | W_1 = V_1, \ldots, W_i = V_i]\\ \label{finished32exploration} & \geq \prod_{i = 0}^{\infty} b^{|V_i|} \prod_{y \in V_{i+1}} \max_{x \in V_i} p_{x, y} = b^{|\Lambda'| + |V'|} \prod_{i = 0}^{\infty} \prod_{y \in V_{i+1}} \max_{x \in V_i} p_{x, y}. \end{align}\tag{12}\]

We now claim that \(\sup_{x \in V} \sum_{y \in V \setminus \{x\}} p_{x, y}\) tends to \(0\) as \(C\) tends to infinity, which in turn implies that \(b\) tends to \(1\). For any \(x, y \in V\) with \(J_{x, y} \neq 0\), we have \[\begin{align} p_{x, y} = \int_{|u| \geq C f(J_{x, y})} e^{-\frac{a}{2}|u|^{n}} \, \mathrm{d} \rho_{a}(u) \leq \exp \left( -\frac{a}{2} (Cf(J_{x,y}))^{n} \right) \rho_{a}(\mathbb{R}). \end{align}\] Given \(x,y \in V\) with \(|J_{x, y}| < \delta_f\), we have by [C2] that \(p_{x, y} \leq \rho_{a}(\mathbb{R}) |J_{x, y}|^{\frac{a}{2}C^{n}}\), and we can choose \(C>0\) to be large enough so that \(\rho_{a}(\mathbb{R}) |J_{x, y}|^{\frac{a}{2}C^{n}}\leq \tfrac{|J_{x, y}|}{CM_f}\). Since \(\sum_{y \in V} |J_{x, y}| \leq M_f\), there are at most \(M_f/\delta_f\) vertices \(y\in V\) such that \(|J_{x,y}|\geq \delta_f\) and for these vertices, we can use the bound \(p_{x, y} \leq e^{-a C^{n}/2} \rho_{a}(\mathbb{R})\). The claim follows.

Let \(\alpha_3 = b^{-1} e^{K} \in [1, \infty)\). It follows from summing 12 over \(V_1, V_2, \ldots\) that \[\label{final95bound} \sum_{(V_j)} e^{K(|\Lambda'|+|V'|)}\prod_{i = 0}^{\infty} \prod_{y \in V_{i+1}} \max_{x \in V_i} p_{x, y}\leq \alpha_{3}^{|\Lambda'|} \sum_{k = 0}^{\infty} \alpha_{3}^k \mathbb{P}[|W| = k].\tag{13}\] We want to stochastically dominate \((W_i)_{i \geq 0}\) by a branching process \((Z_i)_{i \geq 0}\). By choosing the value of \(C\) to be large enough, we can ensure that \(b \geq 1/2\). We can then define a random variable \(X\) by \[\mathbb{P}[X = k] = \begin{cases} b &\text{if } k = 0,\\ 1 - b - \frac{(1-b)^2}{b} &\text{if } k = 1, \\ (1-b)^k &\text{if } k \in \{2, 3, \ldots\}, \end{cases}\] and let \((Z_i)_{i \geq 0}\) be a branching process with initial population \(|\Lambda'|\) and offspring distribution \(X\). If \(x \in W_i\) for some \(i \in \{0,1,\ldots\}\), let \(X_x\) be the number of vertices \(y \in W_{i+1}\) such that the edge \(xy\) is open. For all \(k \geq 0\), we have \(\mathbb{P}[X_x \geq k] \leq \mathbb{P}[X_x \ge 1]^k \leq (1-b)^k \leq \mathbb{P}[X \geq k]\), which proves the desired stochastic domination. In particular, since \(\alpha_3 \geq 1\) we have that \[\begin{align} \nonumber \sum_{k = 0}^{\infty} \alpha_{3}^k \mathbb{P}[|W| = k] \leq \sum_{k = 0}^{\infty} \alpha_{3}^k \mathbb{P}[T = k + |\Lambda'|], \end{align}\] where \(T\) is the total progeny of \((Z_i)_{i \geq 0}\). Applying Theorem 4 gives that \[\begin{align} \nonumber \sum_{k = 0}^{\infty} \alpha_{3}^k \mathbb{P}[|W| = k] &\leq \alpha_3^{|\Lambda'|} + \sum_{k = |\Lambda'|}^{\infty} \alpha_{3}^k \frac{|\Lambda'|}{k + |\Lambda'|} \mathbb{P}[X_1 + \ldots + X_{k + |\Lambda'|} = k]\\ \label{sum32of32X321} & \leq \alpha_3^{|\Lambda'|} + \frac{1}{2}\sum_{k = |\Lambda'|}^{\infty} \alpha_3^{k} \mathbb{P}[X_1 + \ldots + X_{2k} \geq k], \end{align}\tag{14}\] where \(X_1, X_2,\ldots\) are independent with the same distribution as \(X\). We now bound the latter probability as follows. Setting \(\theta = 2 \log(2\alpha_3)\), we have that \(\mathbb{E}[e^{\theta X}] \rightarrow 1\) as \(b \rightarrow 1\). By increasing the value of \(C\), we can make \(b\) as close to 1 as desired, so by choosing \(C\) large enough, we can ensure that \(\mathbb{E}[e^{\theta X}] < e^{\theta/4}\). We then have by the exponential Markov inequality and independence \[\label{sum32of32X322} \mathbb{P}[X_1 + \ldots + X_{2k} \geq k] \leq e^{-\theta k} \mathbb{E}[e^{\theta X}]^{2k} \leq e^{-\theta k/2} = (2\alpha_3)^{-k}.\tag{15}\] Combining 14 and 15 yields \[\sum_{k=0}^{\infty} \alpha_{3}^{k} \mathbb{P}[|W| = k] \leq \alpha_3^{|\Lambda'|} + 2^{-|\Lambda'|},\] and substituting this in 13 completes the proof. ◻

Remark 5. In the case of nearest-neighbour interactions on a graph of bounded degree, the proof of Lemma 5 can be simplified by using the fact that the number of ways to choose \(\mathcal{C} \setminus \Lambda'\) so that \(|\mathcal{C} \setminus \Lambda'| = k\) is at most exponential in \(k+|\Lambda'|\).

4 Regularity for related models↩︎

In this section, we aim to generalise Theorem 1. We first show that our arguments can also be applied when \(\rho\) satisfies 3 with \(n=2\) for some \(a \geq 4 \beta M_f\), with the other assumptions from Section 2.1 unchanged.

Recall from Section 2.2 the definition of \(A(x, \Lambda)\) in the case \(n=2\). The assumption that \(a \geq 4 \beta M_f\) is stronger than is necessary for our arguments or the arguments of [1] to apply, but in later applications we only consider the case when \(\rho\) satisfies 2 , so we include this assumption for simplicity. The theorem below is the analogue of Theorem 1 in the case \(n=2\).

Theorem 6. Let \(a\geq 4 \beta M_f\) and assume \(\rho\) satisfies \(\int_{\mathbb{R}} e^{a |u|^{2}} \mathrm{d} \rho(u) < \infty\). There exist \(C \geq 1, \tilde{C} > 0\) depending only on \(\beta, \delta_f, M_f, \rho\) and \(a\) such that for any \(\Lambda \Subset V\), \(\Lambda' \subset \Lambda\), \(\psi \in \mathbb{R}^{\Lambda'}\), \(\lambda\leq \frac{a}{4 \beta M_f}\), and any boundary conditions \(\xi \in \mathbb{R}^{V}\) with \(\sum_{y \in V} |J_{x, y} \xi_y| < \infty\) for all \(x \in \Lambda\), \[\mathrm{d} \nu_{\Lambda, \beta, \rho, J}^{\xi}[\varphi|_{\Lambda'} = \psi] \leq \prod_{x \in \Lambda'} e^{\tilde{C} A(x, \Lambda, \xi, C)^2} \mathrm{d} \nu_{\Lambda', 0, \rho_{\frac{a}{2}}, 0}^{0} [\psi].\]

When \(\rho\) satisfies 2 , it follows from Theorem 6 that we have tightness for any boundary conditions that are in \(\Xi(\lambda)\) for some \(\lambda \geq 1\). For nearest-neighbour interactions on a graph \(G\), this includes exponentially growing boundary conditions of the form \(|\xi_x| \leq C \lambda^{d_G(o, x)}\) (see 23 ), so we observe that the threshold for tightness jumps from exponential when \(n=2\) to double exponential when \(n > 2\).

The proof of Theorem 6 is essentially the same as that of Theorem 1 but with different definitions of \(\mathcal{C}\) and \(A\).

Proof of Theorem 6. Fix a finite subset \(\Lambda \subset V\) and let \(\Lambda' \subset \Lambda\). We write \(E\) for \(\{xy \in \overline{E}(\Lambda, J): x,y \in \Lambda\}\) and \(A_x\) for \(A(x, \Lambda, \lambda, \xi, C, J, f)\), where \(C \geq 1\) is a constant to be determined. Define \(\mathcal{C}\) to be the set of vertices \(x \in \Lambda\) such that for some \(m \in \{ 0, 1, \ldots\}\) there exists a walk \(x_0, x_1, \ldots, x_m\) from \(\Lambda'\) to \(x\) in \(\overline{(\Lambda, J)}\) that satisfies \[\label{cluster32membership32criteria32n612} \forall k \in S_m \quad |\varphi_{x_k}| \geq C A_{x_0} \lambda^{k} \prod_{i = 1}^{k} f(J_{x_{i-1}, x_i}),\tag{16}\] where \(S_0 = \{0\}\) and \(S_m = \{1, \ldots, m\}\) for \(m \geq 1\). For each \(i \in \{ 0, 1, \ldots\}\), let \(\mathcal{C}_i\subset \mathcal{C}\) denote the set of vertices for which \(i\) is the smallest value of \(m\) such that there exists a walk satisfying 16 . Let \(\alpha_0 \geq 1\) be such that \(\rho_{a}([-\alpha_0, \alpha_0]) > 0\). Given \((\mathcal{C}_i)_{i \geq 1} = (V_i)_{i \geq 1}\) with \(\bigcup_{i = 1}^{\infty} V_i = V'\), let \(t \in [-\alpha_0, \alpha_0]^{\Lambda' \cup V'}\) and define the configuration \(\tilde{\varphi} \in \mathbb{R}^{\Lambda}\) as in the proof of Theorem 1. Setting \(\alpha_1 = \frac{a C^{2}}{2 M_f} \geq 2 \beta C^{2} \lambda\), one can show that when \(C \geq \alpha_0\) \[\begin{align} \label{compactified32inequality32n612} &\beta J_{x,y} \varphi_x \varphi_y \leq\\ \nonumber &\beta J_{x,y} \tilde{\varphi}_x \tilde{\varphi}_y +|J_{x,y}|f(J_{x, y}) \left(\frac{a|\varphi_x|^{2}}{2M_f}\mathbb{1}_{x\in \mathcal{C}}+\alpha_1 A_x^2 \mathbb{1}_{x\in \Lambda' \setminus \mathcal{C}}+\frac{a|\varphi_y|^{2}}{2M_f}\mathbb{1}_{y\in \mathcal{C}}+\alpha_1 A_x^2 \mathbb{1}_{y\in \Lambda' \setminus \mathcal{C}} \right), \end{align}\tag{17}\] and \[\label{compactified32inequality3223240n61241} \beta h_{x,\Lambda} \varphi_x \leq \beta h_{x, \Lambda} \tilde{\varphi}_x + \left( \frac{a|\varphi_x|^2}{2M_f}\mathbb{1}_{x\in \mathcal{C}}+\alpha_1 A_x^2 \mathbb{1}_{x\in \Lambda' \setminus \mathcal{C}} \right) \sum_{y \in V \setminus \Lambda} |J_{x, y}| f(J_{x,y}).\tag{18}\] The first inequality 17 can be verified in a similar way to 7 . Indeed, if \(|\varphi_x|, |\varphi_y| \geq \alpha_0\), then applying Lemma 2 and using that \(a \geq 4 \beta M_f\) gives that \[\begin{align} \beta (|\varphi_x| |\varphi_y| + |t_x||t_y|) \leq \frac{a f(J_{x,y})}{2M_f} (|\varphi_x|^{2} + |\varphi_y|^{2}). \end{align}\] We also use that if \(x\in \mathcal{C}\) and \(y\in \Lambda\setminus \mathcal{C}\), then \(|\varphi_x| \geq \alpha_0\) and \(|\varphi_y| \leq \lambda f(J_{x,y}) |\varphi_x|\), which implies \[\begin{align} \label{Edge32removal32alt32n6123240i41} \beta (|\varphi_x| |\varphi_y| + |t_x||\varphi_y|) \leq 2 \beta \lambda f(J_{x,y}) |\varphi_x|^{2} \leq \frac{a f(J_{x,y})}{2M_f} |\varphi_x|^{2}. \end{align}\tag{19}\] To prove 18 , if \(x \in \mathcal{C}\) then \[\begin{align} |h_{x, \Lambda}|\leq \left(\sum_{y \in V \setminus \Lambda} |J_{x, y}| f(J_{x,y}) \right) \lambda |\varphi_x|, \end{align}\] so 19 applies. If \(x \in \Lambda' \setminus \mathcal{C}\) then we bound \(|h_{x, \Lambda}|\) using the definition of \(A_{x}\) to obtain \[|h_{x, \Lambda}| \leq C \lambda A_x \left(\sum_{y \in V \setminus \Lambda} |J_{x, y}| f(J_{x,y}) \right).\] Having obtained 17 and 18 , we use Lemmas 4 and 5 as in the proof of Theorem 1 to conclude. ◻

Remark 7. Theorem 6 can be generalised by allowing the single-site measure to depend on the vertex. We will use such a generalisation to construct the infinite-volume plus measure as the limit of systems with a shifted single-site measure at the boundary.

Suppose the single-site measure at vertex \(x\) is given by \(d\rho_{x, \Lambda}(u) = e^{-a_{x, \Lambda}|u|^2}d\mu_{x, \Lambda}(u)\) and there exist a bounded subset \(T \subset \mathbb{R}\) and constants \(a_{\min}, a_{\max}, M_1, M_2 >0\) such that for all \(\Lambda \Subset V\) and \(x \in \Lambda\),

  1. \(a_{\min} \leq a_{x, \Lambda} \leq a_{\max}\),

  2. \(\mu_{x, \Lambda}(T) \geq M_1\),

  3. \(\mu_{x, \Lambda}(\mathbb{R}) \leq M_2\).

Then there exist \(C \geq 1, \tilde{C} > 0\) such that for any \(\Lambda \Subset V\), \(\Lambda' \subset \Lambda\), \(\psi \in \mathbb{R}^{\Lambda'}\), \(\lambda\leq \frac{a_{\min}}{4 \beta M_f}\), and any boundary conditions \(\xi \in \mathbb{R}^{V}\) with \(\sum_{y \in V} |J_{x, y} \xi_y| < \infty\) for all \(x \in \Lambda\), \[\mathrm{d} \nu_{\Lambda, \beta, \rho, J}^{\xi}[\varphi|_{\Lambda'} = \psi] \leq \left( \prod_{x \in \Lambda'} e^{\tilde{C} A(x, \Lambda, \xi, C)^{2}} \right) \mathrm{d} \nu_{\Lambda', 0, \tilde{\rho}, 0}^{0} [\psi],\] where \(\tilde{\rho}\) is given by \(d\tilde{\rho}_{x}(u) = e^{-\frac{1}{2}a_{x, \Lambda}|u|^2}d\mu_{x, \Lambda}(u)\).

Assumption [A2] is used in 11 while assumptions [A1] and [A3] are used to bound \[\label{changed32pxy32def} p_{x,y} = \int_{|u| \geq C f(J_{x,y})} e^{-\frac{a_{y, \Lambda}}{2}} \mathrm{d} \mu_{y, \Lambda}(u)\qquad{(2)}\] for \(J_{x,y} \neq 0\). Theorem 1 also holds for any single site measures satisfying [A1], [A2], [A3].

Changing the Hamiltonian can also be considered. We will still restrict our attention to pairwise interactions and will assume further that interactions occur only between neighbours on a graph with bounded degree, so there is an upper bound on the number of vertices that any given vertex can interact with.

Let \(G=(V, E)\) be a graph with bounded degree. For \(\Lambda \Subset V\) and boundary conditions \(\xi \in \mathbb{R}^{V}\), define the measure \(\nu_{\Lambda, U, \rho}^{\xi}\) by \[\mathrm{d} \nu_{\Lambda, U, \rho}^{\xi}[\varphi] = \frac{1}{Z_{\Lambda, U, \rho}^{\xi}} \prod_{\substack{xy \in E\\x, y \in \Lambda}} U_{xy}(\varphi_x, \varphi_y) \prod_{\substack{xy \in E\\x \in \Lambda, y \in V \setminus \Lambda}} U_{xy}(\varphi_x, \xi_y) \prod_{x \in \Lambda} \mathrm{d} \rho_{x, \Lambda}(\varphi_x),\] for \(\varphi \in \mathbb{R}^{\Lambda}\), where \(Z_{\Lambda, U, \rho}^{\xi}\) is the partition function and for each \(xy \in E\), \(U_{xy}: \mathbb{R}^{2} \rightarrow \mathbb{R}^{+}\) is a function.

Theorem 8. Let \(D \geq 1\) and let \(G=(V, E)\) be a graph such that \(\mathrm{deg}(x) \leq D\) for all \(x \in V\). Let \(\rho_{x, \Lambda}\) be single-site measures satisfying 2 and assumptions [A1],[A2],[A3]. For each \(xy \in E\), let \(U_{xy}: \mathbb{R}^{2} \rightarrow \mathbb{R}^{+}\) be a function satisfying the following assumptions for some constants \(C \geq 1\), \(\lambda \geq 1\), and function \(F: [1, \infty) \rightarrow [1, \infty)\):

(i) If \(|\varphi_x| \geq C\), \(t_x\in T\) and \(|\varphi_y| \leq \lambda |\varphi_x|\), then \[U_{xy}(\varphi_x, \varphi_y) \leq U_{xy}(t_x, \varphi_y) \exp\left(\frac{a_{x, \Lambda}}{2D}|\varphi_x|^{2}\right).\]

(ii) If \(t_x,t_y\in T\) and \(|\varphi_x| \leq C A_x, |\varphi_y| \leq C \lambda A_x\) for some \(A_x \geq 1\), then \[\max\left\{ \frac{U_{xy}(t_x, \varphi_y)}{U_{xy}(t_x, t_y)}, \frac{U_{xy}(\varphi_x, \varphi_y)}{U_{xy}(t_x, t_y)}, \frac{U_{xy}(\varphi_x, \varphi_y)}{U_{xy}(t_x, \varphi_y)} \right\} \leq e^{F(A_x)}.\]

Then there exist constants \(C_1, C_2\) such that for any \(\Lambda \subset V\) finite, \(\Lambda' \subset \Lambda\), \(\psi \in \mathbb{R}^{\Lambda'}\), and any boundary conditions \(\xi \in \mathbb{R}^{V}\) satisfying \(\sum_{y \in V} |J_{x, y} \xi_y| < \infty\) for all \(x \in \Lambda\), \[\mathrm{d} \nu_{\Lambda, U, \rho}^{\xi}[\varphi|_{\Lambda'} = \psi] \leq \prod_{x \in \Lambda'} \exp \left(C_1 F(A(x, \Lambda, \lambda, \xi, C_2)) -\frac{1}{2} a_{x, \Lambda} |\psi_x|^{2} \right) \mathrm{d} \mu_{x, \Lambda} (\psi_x).\]

Proof of Theorem 8. Let \(f(1) = 1\) and write \(A_x\) for \(A(x, \Lambda, \lambda, \xi, C_2, J, f)\), where \(C_2 \geq 1\) is a constant to be determined. Define \(\mathcal{C}\) to be the set of vertices \(x \in \Lambda\) such that for some \(m \in \{ 0, 1, \ldots\}\) there exists a walk \(x_0, x_1, \ldots, x_m\) from \(\Lambda'\) to \(x\) in \(\overline{(\Lambda, J)}\) that satisfies \[\label{changed32cluster32membership32criteria} \forall k \in S_m \quad |\varphi_{x_k}| \geq C_2 A_{x_0} \lambda^{k},\tag{20}\] where \(S_0 = \{0\}\) and \(S_m = \{1, \ldots, m\}\) for \(m \geq 1\). For each \(i \in \{ 0, 1, \ldots\}\), let \(\mathcal{C}_i\subset \mathcal{C}\) denote the set of vertices for which \(i\) is the smallest value of \(m\) such that there exists a walk satisfying 20 . Given \((\mathcal{C}_i)_{i \geq 1} = (V_i)_{i \geq 1}\) with \(\bigcup_{i = 1}^{\infty} V_i = V'\), let \(t \in T^{\Lambda' \cup V'}\) and define the configurations \(\varphi', \tilde{\varphi} \in \mathbb{R}^{V}\) by \[\varphi'_x = \begin{cases} \varphi_x & \text{if } x \in \Lambda,\\ \xi_x & \text{otherwise}, \end{cases} \qquad \tilde{\varphi}_x = \begin{cases} t_x & \text{if } x \in \Lambda' \cup V',\\ \varphi'_x & \text{otherwise}. \end{cases}\] Assumption (i) in the statement of the theorem is analogous to 19 , and (ii) allows us to bound \(U_{xy}(\varphi'_x, \varphi'_y)\) in terms of \(U_{xy}(\tilde{\varphi}_x, \tilde{\varphi}_y)\) when \(x\) or \(y\) is in \(\Lambda' \setminus \mathcal{C}\). Together with the definitions of \(\mathcal{C}\) and \(A(o, \Lambda)\), they imply that for any \(xy \in E\) \[\begin{align} &U_{xy}(\varphi'_x, \varphi'_y) \leq\\ &U_{xy}(\tilde{\varphi}_x, \tilde{\varphi}_y) \exp\left(\frac{a_{x, \Lambda}}{2D}|\varphi_x|^{2} \mathbb{1}_{x \in \mathcal{C}} + F(A_{x}) \mathbb{1}_{x \in \Lambda' \setminus \mathcal{C}} + \frac{a_{y, \Lambda}}{2D}|\varphi_y|^{2} \mathbb{1}_{y \in \mathcal{C}} + F(A_{y}) \mathbb{1}_{y \in \Lambda' \setminus \mathcal{C}}\right). \end{align}\] Combining over all edges and using that each vertex has degree at most \(D\), we get \[\begin{align} \prod_{xy \in E} U_{xy}(\varphi'_x, \varphi'_y) \leq \left(\prod_{xy \in E} U_{xy}(\tilde{\varphi}_x , \tilde{\varphi}_y) \right) \prod_{x \in \mathcal{C}} e^{\frac{a_{x, \Lambda}}{2}|\varphi_x|^{2}} \prod_{x \in \Lambda'} e^{D F(A_{x})}. \end{align}\] By combining the above with the terms coming from the single-site measure and integrating, we can show as in the proof of Lemma 4 that for some \(K\geq0\), \[\begin{align} &\mathrm{d}\nu_{\Lambda, U, \rho}^{\xi} \left[ \varphi|_{\Lambda'}, \, (\mathcal{C}_i)_{i \geq 1} = (V_i)_{i \geq 1} \right] \leq \\ \nonumber &\exp \left(K|\Lambda'\cup V'| \right) \left( \prod_{x \in \Lambda'} e^{DF(A_x)} e^{\frac{-a_{x, \Lambda}}{2}|\varphi_x|^2} \mathrm{d}\mu_{x, \Lambda}(\varphi_x) \right) \prod_{i = 0}^{\infty} \prod_{y \in V_{i+1}} \max_{x \in V_i} p_{x, y}, \end{align}\] with \(p_{x,y}\) defined as in ?? . Applying Lemma 5 concludes the proof. ◻

Remark 9. One example where Theorem 8 is useful is the random cluster representation of the \(\varphi^{4}\) model, introduced in [13], which is a measure on pairs \((\mathsf{a},\omega)\), where \(\mathsf{a}\) is the absolute value field and \(\omega\) is a percolation configuration. We may wish to consider the distribution of \(\mathsf{a}\) in this model conditional on observing a given percolation configuration \(\omega\), similarly to [13]. In this case, the functions \(U_{xy}\) are given by \[U_{xy}(\mathsf{a}_x, \mathsf{a}_y) = \begin{cases} e^{-\beta \mathsf{a}_x \mathsf{a}_y} & \text{if } \omega_{xy} = 0,\\ e^{\beta \mathsf{a}_x \mathsf{a}_y} - e^{-\beta \mathsf{a}_x \mathsf{a}_y} & \text{if } \omega_{xy} = 1. \end{cases}\] We now check that assumptions (i) and (ii) in Theorem 8 are satisfied and that the choice of \(C, \lambda\) and \(F\) does not depend on \(\omega\). Assume \(\rho_{x, \Lambda}\) are single-site measures supported on \(\mathbb{R}^{+}\) that satisfy the assumptions of Theorem 8 and let \(\lambda = \frac{a_{\min}}{4 D \beta}\). Let \(C\geq 1\) be a constant to be determined and let \(T = [t_{\min}, t_{\max}]\), where \(0 <t_{\min} < t_{\max} \leq C\) and \(T\) satisfies [A2]. Let \(xy \in E\). If \(\omega_{xy} = 0\), then the interaction term \(U_{xy}(\mathsf{a}_x, \mathsf{a}_y)\) is of the same form as in Theorem 6, so (i) follows from 19 . Now suppose \(\omega_{xy} = 1\) and observe that since the spins \(\mathsf{a}_x\) only take positive values in this model, \(U_{xy}\) is increasing in both arguments. Note that if \(\mathsf{a}_x \geq C \geq t_x \ge t_{\min}\) and \(\mathsf{a}_y \leq \lambda \mathsf{a}_x\), then \(\frac{U_{xy} (\mathsf{a}_x, \mathsf{a}_y)}{U_{xy}(t_x, \mathsf{a}_y)}\) is an increasing function of \(\mathsf{a}_y\). Hence, \[\begin{align} \frac{U_{xy} (\mathsf{a}_x, \mathsf{a}_y)}{U_{xy}(t_x, \mathsf{a}_y)} \leq \frac{U_{xy} (\mathsf{a}_x, \lambda \mathsf{a}_{x})}{U_{xy}(t_x, \lambda \mathsf{a}_x)} \leq \frac{\exp(\beta \lambda \mathsf{a}_x^{2})}{U_{xy}(t_{\min}, C \lambda)}. \end{align}\] The choice of \(\lambda\) implies the right hand side above is at most \(\exp\left(\frac{a_{\min}}{2D}\mathsf{a}_x^{2}\right)\) for all \(C\) large enough, so (i) holds. For (ii), we use that if \(\omega_{xy} = 1\), the maximum in (ii) is at most \[\frac{U_{xy}(CA_{x}, C\lambda A_{x})}{U_{xy}(t_{\min}, t_{\min})},\] and if \(\omega_{xy} = 0\) then it is at most \(\exp(2\beta C^2 \lambda A_{x}^{2})\) by 17 .

5 Corollaries and applications↩︎

In this section, we give some examples of interactions \(J\) and boundary conditions \(\xi\) for which we can apply our regularity results, and we then apply them to construct infinite volume measures. Recall from Section 2.2 that \(\Xi\) is the set of boundary conditions \(\xi\) for which \(\tilde{A}(x, V, \xi) < \infty\) for all \(x \in V\), and that we have tightness for any \(\xi \in \Xi\). For nearest-neighbour interactions, we will give a full characterisation of \(\Xi\) and show for certain choices of \(\rho\) that \(\xi \in \Xi\) is necessary to obtain tightness in the case of non-negative boundary conditions. We also give examples of boundary conditions that are in \(\Xi\) for different forms of long-range interactions. Later we give conditions on \(\xi\) that ensure the measures \(\nu_{\Lambda, \beta, \rho, J}^{\xi}\) converge to an \(a\)-regular Gibbs measure as \(\Lambda \nearrow V\) and construct the extremal regular Gibbs measures \(\nu^{+}\) and \(\nu^{-}\).

We begin by defining some notation that will be used throughout this section. Assume \(G = (V, E)\) is an infinite connected graph such that every vertex has finite degree, and fix an origin \(o \in V\). Let \(d_G: V \times V \rightarrow \mathbb{N}_{0}\) be the graph distance in \(G\), and for \(S \subset V\) let \(d_S\) denote the graph distance in the subgraph of \(G\) induced by \(S\). For \(x \in V\), let \(\mathrm{deg}(x)\) be the degree of \(x\) in the graph \(G\).

5.1 Results for nearest-neighbour interactions↩︎

We first consider the case of (ferromagnetic) nearest-neighbour interactions, which are defined as follows when \(G\) has bounded degree.

Definition 4. If there exists a constant \(D\) such that \(\mathrm{deg}(x) \leq D\) for all \(x \in V\), then we define nearest-neighbour interactions \(J_G\) on \(G\) by \[(J_G)_{x, y} = \begin{cases} 1 & \text{if } xy \in E,\\ 0 & \text{otherwise}. \end{cases}\]

In the nearest-neighbour case, we may choose \(f\) to be so that \(f(1) = 1\). Then, in the \(n>2\) case, \[A(x, R) = \max \left\{ 1, \max_{y \in \partial R} \left(\frac{|h_{y,R}|}{C|N_{y, V\setminus R}|}\right)^{(n-1)^{-d_R(x,y) -1}} \right\},\] where \(N_{y, V\setminus R} = \{z \in V \setminus R : d_G(y,z) = 1\}\) and \(\partial R = \{y \in R: N_{y, V\setminus R} \neq \emptyset\}\). We also have \[\tilde{A}(x, R) = \max \left\{ 1, \max_{z \in V} \left(\frac{|\xi_z|}{C}\right)^{(n-1)^{-d_{R \cup \{z\}}(x, z)}} \right\}.\] As a consequence of this and connectedness, it follows from Lemma 1 that \[\label{eq:32short32range32Xi} \Xi = \{\xi \in \mathbb{R}^{V} : \exists \;A_{\xi} \in (0, \infty) \text{ such that } |\xi_z| \leq A_{\xi}^{(n-1)^{d_G(o, z)}} \, \forall \, z \in V\}.\tag{21}\]

In the \(n=2\) case, we have \[\label{eq:32formula32for32A32n612} A(x, R) = \max \left\{ 1, \max_{y \in \partial R} \left(\frac{|h_{y,R}|}{C|N_{y, V\setminus R}|\lambda^{d_R(x,y)+1}}\right) \right\},\tag{22}\] and \[\tilde{A}(x, R) = \max \left\{ 1, \max_{z \in V} \left(\frac{|\xi_z|}{C\lambda^{d_{R \cup \{z\}}(x, z)}}\right) \right\},\]

so that \[\label{eq:32short32range32Xi32n612} \Xi(\lambda) = \{\xi \in \mathbb{R}^{V} : \exists \;C_{\xi} \in (0, \infty) \text{ such that } |\xi_z| \leq C_{\xi}\lambda^{d_G(o, z)} \, \forall \, z \in V\}.\tag{23}\]

The remainder of the subsection is devoted to justifying that our regularity results are optimal. More precisely, we aim to show that for the \(P(\varphi)\) models, any non-negative boundary conditions for which we have tightness are in \(\Xi\). To simplify the calculations, we only consider the case when \(P(u) = \tilde{a}|u|^{n}\) here. Note that in this case \(\rho\) satisfies 3 for any \(a < \tilde{a}\).

Proposition 10. Assume \(n>2, \tilde{a} > 0\), \(\mathrm{d} \rho(u) = e^{-\tilde{a}|u|^{n}} \mathrm{d} u\) and \(G\) has bounded degree. If \(\xi \in (\mathbb{R}^{+})^{V} \setminus \Xi\), then the family of measures \((\nu_{\Lambda, \beta, \rho, J_G}^{\xi})_{\Lambda \Subset V}\) is not tight.

When \(V = \mathbb{Z}\) we can obtain the same result as Proposition 10 for mixed positive and negative boundary conditions.

Proposition 11. Assume \(n>2, \tilde{a} > 0\), \(\mathrm{d} \rho(u) = e^{-\tilde{a}|u|^{n}} \mathrm{d} u\) and \(G = (\mathbb{Z}, \{xy : |x-y| = 1\})\). If \(\xi \in \mathbb{R}^{\mathbb{Z}} \setminus \Xi\), then the family of measures \((\nu_{\Lambda, \beta, \rho, J_G}^{\xi})_{\Lambda \Subset V}\) is not tight.

In the proofs of the above propositions, we will use the following monotonicity property.

Lemma 6. Assume \(\rho\) is an even measure satisfying 3 . Suppose \(J, J'\) are interactions on \(V\) satisfying [C1], [C2] and \(0 \leq J_{x, y} \leq J'_{x,y}\) for all \(x, y \in V\). Suppose also that \(\xi, \xi'\) are boundary conditions on \(\Lambda\) such that \(0 \leq \xi_x \leq \xi'_x\) for all \(x \in V\) and \(\sum_{y \in V} J'_{x, y} |\xi'_y| < \infty\) for all \(x \in \Lambda\). Let \(u\geq 0\) and \(x \in \Lambda\). Then \[\nu_{\Lambda, \beta, \rho, J}^{\xi}[\varphi_x \geq u] \leq \nu_{\Lambda, \beta, \rho, J'}^{\xi'}[\varphi_x \geq u].\]

Proof. Monotonicity in \(\xi\) has already been established in Proposition 3, so we just need to prove that \(\nu_{\Lambda, \beta, \rho, J}^{\xi}[\varphi_x \geq u] \leq \nu_{\Lambda, \beta, \rho, J'}^{\xi}[\varphi_x \geq u]\). Writing \(\sigma_x\) for the sign of \(\varphi_x\) and using that \(\mathbb{1}_{\{\sigma_x = 1\}} = \frac{1}{2}(1 + \sigma_x)\), we have \[\begin{align} \nu_{\Lambda, \beta, \rho, J}^{\xi}[\varphi_x \geq u] &= \nu_{\Lambda, \beta, \rho, J}^{\xi}[|\varphi_x| \geq u] \nu_{\Lambda, \beta, \rho, J}^{\xi}[\sigma_x = 1 \mid |\varphi_x| \geq u]\\ &= \frac{1}{2} \nu_{\Lambda, \beta, \rho, J}^{\xi}[|\varphi_x| \geq u] (1 +\langle \sigma_x \mid |\varphi_x| \geq u \rangle_{\Lambda, \beta, \rho, J}^{\xi}). \end{align}\] Conditional on the absolute value field, \(\sigma\) is distributed according to an Ising model with coupling constants determined by the absolute value field. As the boundary conditions are positive, monotonicity of the Ising model in \(J\) follows by differentiating and using Griffiths’ inequality [6], and monotonicity of the absolute value field was proved in [13]. ◻

We are now ready to proceed with the proofs of Propositions 10 and 11.

Proof of Proposition 10. Using the characterisation 21 of \(\Xi\), \(\xi \in (\mathbb{R}^{+})^{V} \setminus \Xi\) implies that there exists a sequence of vertices \((z_i)_{i \geq 1}\) such that \(\xi_{z_i}^{(n-1)^{-m_i}} \rightarrow \infty\) as \(i \rightarrow \infty\), where \(m_i = d_G(o, z_i)\). Since there are only finitely many vertices at any fixed distance from \(o\), by passing to a subsequence, we may assume that \(1 \leq m_i < m_j\) for any \(i < j\). Given \(i \geq 1\), let \(\Lambda_i = \{ x \in V : d_G(o, x) < m_i\}\) and let \(y_{i,0}, y_{i,1}, \ldots, y_{i,m_i}\) be a walk from \(o\) to \(z_i\) in \(\overline{(\Lambda_i, J)}\). Also let \(\alpha = \frac{\beta}{\tilde{a}n2^{n-1}}\), and for \(j \in \{0, \ldots, m_i\}\), define \[D_{i, j} = \alpha^{\frac{1-(n-1)^{j-m_i}}{n-2}} \xi_{z_i}^{(n-1)^{j - m_i}}.\] Then \(D_{i, m_i} = \xi_{z_i}\) and \(D_{i, j+1} = \alpha^{-1} D_{i, j}^{n-1}\). We will show that there exists \(\varepsilon > 0\) such that for all \(i\) sufficiently large, \(\nu_{\Lambda_i, \beta, \rho, J_G}^{\xi} [\varphi_o \geq D_{i, 0}] \geq \varepsilon\). Since \(D_{i, 0} \geq \min \{1, \alpha^{\frac{1}{n-2}}\} \xi_{z_i}^{(n-1)^{-m_i}} \rightarrow \infty\) as \(i \rightarrow \infty\), this implies that the sequence is not tight. The strategy for the proof is to condition in turn on the events \(\{ \varphi_{y_{i,j}} \geq D_{i, j} \}\). We can then use Lemma 6 to set \(J_{x, y} = 0\) everywhere except for the edge between \(y_{i,j}\) and \(y_{i,j+1}\), meaning that we only have to calculate a one-dimensional integral in each step. We have \[\begin{align} \nu_{\Lambda_i, \beta, \rho, J_G}^{\xi}[\varphi_{o} \geq D_{i,0}] &\geq \nu_{\Lambda_i, \beta, \rho, J_G}^{\xi} [\varphi_{y_{i,j}} \geq D_{i,j} \; \forall j \in \{0, \ldots, m_i - 1\}]\\ &= \prod_{j = 0}^{m_i - 1} \nu_{\Lambda_i, \beta, \rho, J_G}^{\xi} [\varphi_{y_{i,j}} \geq D_{i, j} \mid \varphi_{y_{i,k}} \geq D_{i,k} \; \forall k \in \{j+1, \ldots, m_i - 1\}]. \end{align}\] Define \(J^{(i,j)}\) by \((J^{(i,j)})_{x, y} = 1\) if \(\{x, y\} = \{y_{i,j}, y_{i, j+1}\}\) and \((J^{(i,j)})_{x, y} = 0\) otherwise. Also let \(\xi^{(i, j)}\) be defined by \(\xi^{(i,j)}_{y_{i, j+1}} = D_{i, j+1}\) and \(\xi^{(i,j)}_{x} = 0\) for all \(x \in V \setminus \{y_{i, j+1}\}\). Using the domain Markov property and Lemma 6, we have \[\nu_{\Lambda_i, \beta, \rho, J_G}^{\xi} [\varphi_{y_{i,j}} \geq D_{i, j} \mid \varphi_{y_{i,k}} \geq D_{i,k} \; \forall k \in \{j+1, \ldots, m_i - 1\}] \geq \nu_{\{y_{i, j}\}, \beta, \rho, J^{(i,j)}}^{\xi^{(i,j)}} [\varphi_{y_{i,j}} \geq D_{i, j}].\] We now estimate the probability on the right hand side. Let \(r = \beta D_{i, j+1} \varphi_{y_{i,j}} - \tilde{a}|\varphi_{y_{i,j}}|^{n}\). Then \[\frac{\mathrm{d} r}{\mathrm{d} \varphi_{y_{i,j}}} \bigg|_{\varphi_{y_{i,j}} = D_{i, j}} = \beta D_{i, j+1} - \tilde{a}n D_{i, j}^{n-1} = \beta D_{i, j+1} \left(1 - \frac{1}{2^{n-1}} \right),\] where the second equality is from our choice of \(\alpha\). This is greater than 1 for all \(j\) if \(i\) is large enough. Then because \(r\) is a concave function of \(\varphi_{y_{i,j}}\), \(\frac{\mathrm{d} r}{\mathrm{d} \varphi_{y_{i,j}}} \geq 1\) whenever \(\varphi_{y_{i,j}} \leq D_{i, j}\). Hence, \[\begin{align} \label{denominator32integral} \int_{- \infty}^{D_{i, j}} e^{\beta D_{i, j+1} \varphi_{y_{i,j}} - \tilde{a}|\varphi_{y_{i,j}}|^{n}} \mathrm{d} \varphi_{y_{i,j}} \leq \int_{- \infty}^{\beta D_{i, j} D_{i, j+1} - \tilde{a} (D_{i, j})^{n}} e^{r} \mathrm{d} r = \exp(\beta D_{i, j} D_{i, j+1} - \tilde{a} (D_{i, j})^{n}). \end{align}\tag{24}\] Note that the maximum value of \(r\) occurs when \(\varphi_{y_{i,j}} = (\frac{\beta}{\tilde{a}n} D_{i, j+1})^{1/(n-1)} = 2 D_{i, j}\), and \(r\) is increasing when \(\varphi_{y_{i, j}} < 2 D_{i, j}\). Consequently, when \(\varphi_{y_{i,j}} \in [D_{i, j}, 2 D_{i,j}]\), the value of \(r\) is at least \(\beta D_{i, j} D_{i, j+1} - \tilde{a} (D_{i, j})^{n}\), which implies \[\begin{align} \label{numerator32integral} \int_{D_{i, j}}^{\infty} e^{\beta D_{i, j+1} \varphi_{y_{i,j}} -\tilde{a}|\varphi_{y_{i,j}}|^{n}} \mathrm{d} \varphi_{y_{i,j}} \geq D_{i, j} \exp(\beta D_{i, j} D_{i, j+1} - \tilde{a} (D_{i, j})^{n}). \end{align}\tag{25}\] Combining 24 and 25 we obtain that \[\nu_{\{y_{i,j}\}, \beta, \rho, J^{(i,j)}}^{\xi^{(i,j)}} [\varphi_{y_{i,j}} \geq D_{i, j}] \geq \frac{D_{i, j}}{D_{i, j} + 1}.\] To conclude, we need to take the product over \(j\) and verify that this is bounded below for all \(i\) sufficiently large by a positive constant that does not depend on \(i\). We have \[\begin{align} \nu_{\Lambda_i, \beta, \rho, J_G}^{\xi}[\varphi_{o} \geq D_{i,0}] \geq \prod_{j = 0}^{m_i - 1} \frac{D_{i, j}}{D_{i, j} + 1} = \exp \left( \sum_{j = 0}^{m_i - 1} \log(D_{i, j}) - \log(D_{i, j} + 1) \right). \end{align}\] Taylor expanding \(\log(D_{i, j} + 1)\) around \(D_{i, j}\), we get \(\log(D_{i, j} + 1) \leq \log(D_{i, j}) + \frac{1}{D_{i, j}}\), so \[\begin{align} \nu_{\Lambda_i, \beta, \rho, J_G}^{\xi}[\varphi_{o} \geq D_{i,0}] \geq \exp \left(- \sum_{j=0}^{m_i -1} \frac{1}{D_{i,j}} \right) \geq \exp \left( -\sum_{j=0}^{\infty} \frac{1}{\min\{ 1, \alpha^{\frac{1}{n-2}}\} (\xi_{z_i}^{(n-1)^{-m_i}})^{(n-1)^{j}}} \right). \end{align}\] Since \(\xi_{z_i}^{(n-1)^{-m_i}} \rightarrow \infty\) as \(i \rightarrow \infty\), The last sum above converges for all \(i\) sufficiently large and decreases to \(0\) as \(i \rightarrow \infty\), from which the desired result follows. ◻

Proof of Proposition 11. If \(\xi \notin \Xi\), then using 21 there exists a sequence of vertices \((z_i)_{i \geq 1}\) such that \(|\xi_{z_i}|^{(n-1)^{-|z_i|}} \rightarrow \infty\) as \(i \rightarrow \infty\). We will proceed with the proof in the case where for infinitely many \(i\), \(z_i\) and \(\xi_{z_i}\) are positive (the other cases are similar). By taking an appropriate subsequence, we can assume that \(\xi_{z_i} \geq 0\) and \(1 \leq z_i < z_j\) for all \(1 \leq i < j\).

Define \(\Lambda_i = \{x \in \mathbb{Z} : |x| < z_i \}.\) We first consider the case when there exists a subsequence \((z_{i_{k}})_{k \geq 1}\) such that \(\xi_{-z_{i_k}} < -\xi_{z_{i_k}}\) for all \(k \geq 1\), which implies that \(\nu_{\Lambda_{i_k}, \beta, \rho, J_G}^{\xi}[\varphi_0 \leq 0] \geq \frac{1}{2}\). To see why this is true, note that if \(\xi_{-z_{i_k}} = -\xi_{z_{i_k}}\), then \(\varphi_0\) and \(-\varphi_0\) have the same distribution, so the probability that \(\varphi_0\) is negative is \(1/2\). Now reducing \(\xi_{-z_{i_k}}\) increases the probability of the event \(\{\varphi_0\leq 0\}\) by Proposition 3.

Conditionally on \(\{\varphi_0 \leq 0\}\), the subgraph \(\{-1, -2, \ldots, -(z_{i_k} -1)\}\) has non-positive boundary conditions. Hence \(-\varphi\) is distributed according to a measure with non-negative boundary conditions, and we can apply Proposition 10 to deduce that there exists \(\varepsilon > 0\) such that \(\nu_{\Lambda_{i_k}, \beta, \rho, J_G}^{\xi}[\varphi_{-1} \leq -D_k|\varphi_0 \leq 0] \geq \varepsilon\) for all \(k\) sufficiently large, where \(D_k \rightarrow \infty\) as \(k \rightarrow \infty\). It follows that \(\nu_{\Lambda_{i_k}, \beta, \rho, J_G}^{\xi}[|\varphi_{-1}| \geq D_k] \geq \frac{\varepsilon}{2}\), so the sequence of measures \((\nu_{\Lambda_{i_k}, \beta, \rho, J_G}^{\xi})_{k \geq 1}\) is not tight.

If no such subsequence exists, then for all \(i\) large enough we have that \(\xi_{-z_i} \geq - \xi_{z_i}\), so \(\nu_{\Lambda_i, \beta, \rho, J_G}^{\xi}[\varphi_0 \geq 0] \geq \frac{1}{2}.\) We can now conclude the proof similarly using that if \(\varphi_0 \geq 0\) then we have non-negative boundary conditions on the subgraph \(\{1, 2, \ldots, z_{i_k} -1\}\). ◻

5.2 Results for more general interactions↩︎

In this subsection, we determine which boundary conditions are in \(\Xi\) in the case of long-range interactions that satisfy some additional assumptions.

Definition 5. We say that interactions \((J_{x, y})_{x, y \in V}\) are reasonable if they satisfy the following assumptions in addition to [C1] and [C2]:

  • \(V\) is \(J\)-connected.

  • There exists \(r> 0\) such that for all \(x\neq y \in V, \, |J_{x, y}| \leq d_G(x, y)^{-r}\).

  • \(f\) is an even function and is decreasing on \((0, \infty)\).

  • There exists \(c \in (0, 1)\) such that \(f(2^{r} t) \geq c f(t)\) for all \(t \in [0, \infty)\).

Note that this includes the nearest-neighbour interactions \(J_G\) as we are assuming \(G\) is connected. The next proposition gives a sufficient condition to have \(\xi \in \Xi\) when \(J\) is reasonable. Below \(c\) and \(r\) are the constants of Definition 5.

Proposition 12. Suppose that \(J\) is reasonable and \(\xi \in \mathbb{R}^{V}\) is such that there exists \(M_{\xi} \in \mathbb{R}\) with \(|\xi_x| \leq M_{\xi} f(d_G(o, x)^{-r})\) for all \(x \in V \setminus \{o\}\). Then \(\xi \in \Xi(\lambda)\) for any \(\lambda \geq \frac{1}{c}\).

Before proving the proposition, we give two examples where it can be applied. Firstly, the mildest function satisfying the assumption [C2] is the function \(f_1\) given by \[f_1(t) = \begin{cases} \log(|t|^{-1})^{1/2} & \text{if } |t| < e^{-1},\\ 1 & \text{otherwise}. \end{cases}\] Proposition 12 implies that if \(|\xi_x|\) grows at most like \(\sqrt{\log(d_G(o, x))}\), then \(\xi \in \Xi(\lambda)\) for any reasonable \(J\) and \(\lambda\) large enough.

For the second example, we consider \(\mathbb{Z}^{d}\), or any vertex-transitive graph of dimension \(d\). Let \(J\) be translation invariant interactions satisfying \(|J_{x,y}| \leq C_J d_{G}(x, y)^{-d-\varepsilon}\) for all \(x \neq y\), where \(C_J, \varepsilon > 0\) are constants. This is the setting in which the regularity results of [1] and [4] were proved. In this case (after making \(C_J =1\) by changing the value of \(\beta\)), for any \(\alpha < \frac{\varepsilon}{d+\varepsilon}\) we can apply Proposition 12 with \(r = d + \varepsilon\) to the function \(f_\alpha\) given by \[f_\alpha(t) = \begin{cases} |t|^{-\alpha} & \text{if } |t| < 1,\\ 1 & \text{otherwise}. \end{cases}\] This implies that any \(\xi\) with \(|\xi_x| \leq M_{\xi} d_G(x, y)^{\alpha(d+\varepsilon)}\) is in \(\Xi(\lambda)\) for all \(\lambda \geq 2^\varepsilon\), so we have tightness for boundary conditions growing at most like \(d_{G}(o, x)^{\delta}\) for \(\delta < \varepsilon\).

We now give the proof of Proposition 12.

Proof of Proposition 12. Since \(V\) is \(J\)-connected, we just need to show that \(\tilde{A}(o, V, \lambda)\) is finite, as Lemma 1 then implies \(\tilde{A}(x, V, \lambda) < \infty\) for all \(x \in V\). First observe that if \(\lambda \geq \frac{1}{c},\) then the assumptions on \(f\) imply that for any walk in \(\overline{(V, J)}\) consisting of distinct vertices \(x_0, x_1, \ldots, x_m\) with \(m \geq 2\), \[\begin{align} \label{eq:walk32shortening} \lambda f(d_G(x_{m-2}, x_{m-1})^{-r}) f(d_G(x_{m-1}, x_{m})^{-r}) &\geq \lambda f\left(\left(\frac{1}{2} d_{G}(x_{m-2}, x_{m})\right)^{-r}\right)\\ \nonumber &\geq f(d_G(x_{m-2}, x_{m})^{-r}). \end{align}\tag{26}\] Repeatedly applying 26 and using that \(f(J_{x_{i-1}, x_i}) \geq f(d_G(x_{i-1}, x_i)^{-r})\) by Definition 5, we deduce that \[\begin{align} \label{one-step32walk} \lambda^m \prod_{i=1}^{m} f(J_{x_{i-1}, x_i}) \geq \lambda f(d_G(x_{0}, x_{m})^{-r}). \end{align}\tag{27}\] The above inequality is in fact valid for any walk \(x_0, x_1, \ldots, x_m\) with \(m \geq 1\) because repeating a vertex in the walk makes the left hand side of 27 larger. Now consider \(z \in V \setminus \{o\}\) with a walk \(x_0, x_1, \ldots, x_m\) from \(o\) to \(z\) in \(\overline{(V, J)}\). Applying 27 to reduce \(x_0, x_1, \ldots , x_{m}\) to a one-step walk \(o, z\) yields \[\begin{align} |\xi_z| \leq M_{\xi} f(d_G(o, z)^{-r}) \leq M_\xi \lambda^{m} \prod_{i=1}^{m} f(J_{x_{i-1}, x_i}), \end{align}\] so if \(\mathcal{A} \geq \frac{M_{\xi}}{C}\), then \(\mathcal{A}\) satisfies the requirements for \(\tilde{A}(o, V, \lambda)\) for any \(z \in V \setminus \{o\}\). The case \(z = o\) can also be included by increasing the value of \(\mathcal{A}\) further if necessary. ◻

5.3 Results for infinite-volume measures↩︎

In this section, we show how our results can be applied to measures defined on \(\mathbb{R}^{V}\). Recall that \(G = (V, E)\) is an infinite connected graph where every vertex has finite degree and with a fixed origin \(o \in V\). For \(y \in V\), we let \(B_k(y) = \{x \in V : d_{G}(x, y) \leq k\}\). Throughout this section, we assume that \(J, f, \beta\) and \(\rho\) are fixed with \(\rho\) satisfying 2 and that \(V\) is \(J\)-connected. We will also drop \(J\) from the subscripts. If \(\rho\) satisfies the stronger assumption 3 for some \(a >0\), \(n>2\), then slightly stronger versions of some statements in this section can be obtained by using the machinery of Theorem 1 instead of Theorem 6.

Recall from Definition 1 the definitions of \(a\)-regular measures and Gibbs measures. As a corollary of Theorem 6, we obtain regularity when \(\nu\) is a limit of finite-volume measures with boundary conditions growing slowly enough that \(A(x, \Lambda)\) is bounded by a constant for all \(x\) sufficiently far from the boundary of \(\Lambda\).

Corollary 2. Let \((\Lambda_i)_{i \geq 1}\) be a sequence of finite subsets of \(V\) such that \(\Lambda_i \nearrow V\) as \(i \rightarrow \infty\) and assume that the boundary conditions \(\xi\) satisfy for some \(\lambda \geq 1\) \[\label{eq:tempered32boundary32conditions32n612} \exists A_{\max} \in [1, \infty) \text{ such that } \limsup_{\Lambda \nearrow V} A(x, \Lambda, \lambda, \xi) \leq A_{\mathrm{max}} \: \forall x \in V.\qquad{(3)}\] If \(\nu_{\Lambda_i, \beta, \rho}^{\xi}\) converges weakly to a probability measure \(\nu\) as \(i \rightarrow \infty\), then \(\nu\) is an \(a-\)regular Gibbs measure for any \(a \geq 2 \beta M_f \lambda\).

Proof. Fix \(\Lambda' \Subset V\) and \(a \geq 4 \beta M_f \lambda\). By Theorem 6, we have for any \(i\) large enough that \(\Lambda' \subset \Lambda_i\), \[\mathrm{d} \nu_{\Lambda_i, \beta, \rho}^{\xi}[\varphi|_{\Lambda'} = \psi] \leq \left(\prod_{x\in \Lambda'}\exp(\tilde{C} A(x, \Lambda_i, \lambda, \xi)^2)\right) \mathrm{d} \nu_{\Lambda', 0, \rho_{\frac{a}{2}}}^{0} [\psi].\] Taking \(i \rightarrow \infty\) and using ?? , we have that \(\nu\) is \(\frac{a}{2}-\)regular with \(B = \tilde{C} A^2_{\max}\). The fact that \(\nu\) is a Gibbs measure follows from the domain Markov property for the measures \(\nu_{\Lambda_i, \beta, \rho}^{\xi}\). ◻

Let us consider some examples where ?? is satisfied. Let \(x \in V\) and assume that \(\Lambda\) is large enough that \(d_G(x, z) \geq \frac{1}{2} d_G(o, z)\) for any \(z \in V \setminus \Lambda\). For nearest-neighbour interactions, suppose \(\xi \in \Xi(\lambda)\). Then by 23 , there exists \(C_\xi \in (0, \infty)\) such that for any \(z \in V \setminus \Lambda\) \[|\xi_z| \leq C_\xi \lambda^{d_G(o, z)} \leq C_\xi \lambda^{2d_G(x, z)},\] which implies that for any \(y \in \partial \Lambda\), \[\frac{|h_{y,\Lambda}|}{C|N_{y, V\setminus \Lambda}|\lambda^{2(d_\Lambda(x,y)+1)}} \leq \max_{z \in N_{y, V\setminus \Lambda}} \left\{\frac{|\xi_z|}{C \lambda^{2 d_G(x, z)}}\right\} \leq \frac{C_\xi}{C}.\] It follows from 22 that \(A(x, \Lambda, \lambda^2, \xi) \leq \max\{1, C_\xi/C\}\), and since this is true for any \(\Lambda\) large enough, ?? holds with \(\lambda^2\) in place of \(\lambda\).

For reasonable interactions, ?? holds with \(\lambda \geq \frac{1}{c}\) for any boundary conditions satisfying the assumptions of Proposition 12. Indeed, the choice of \(\Lambda\) and the assumptions on \(f\) in Definition 5 imply that for any \(z \in V \setminus \Lambda\), \[\begin{align} f(d_G(x,z)^{-r}) \geq f(2^{r}d_G(o,z)^{-r}) \geq c f(d_G(o,z)^{-r}). \end{align}\] Hence by the assumptions on \(\xi\), we have for any walk \(x_0, \ldots, x_m\) from \(x\) to \(z\) \[\begin{align} \label{eq:32reasonable32A95max} |\xi_z| \leq M_{\xi} f(d_G(o, z)^{-r}) \leq \frac{M_{\xi}}{c}f(d_G(x, z)^{-r}) \leq M_{\xi} \lambda^{m} \prod_{i=1}^{m} f(J_{x_{i-1}, x_i}), \end{align}\tag{28}\] where we have used 27 and the fact that \(f(J_{x_{i-1}, x_i}) \geq f(d_G(x_{i-1}, x_i)^{-r})\) in the last inequality. From 28 we see that \(A(x, \Lambda, \lambda, \xi) \leq \frac{M_{\xi}}{C}\).

We now show how we can use regularity to make sense of “maximal” boundary conditions, which will allow us to construct the infinite-volume plus measure. Define \(\xi^{+} \in \mathbb{R}^{V}\) by \(\xi^{+}_x = \sqrt{\log(|B_{d_G(o, x)}(o)|)}\) and let \(\xi^{-} = - \xi^{+}\). Below \(r\) and \(c\) are as in Definition 5.

Proposition 13. Assume the interactions \(J\) are reasonable and ferromagnetic. Suppose also that there exists a constant \(c_0 > 0\) such that for any \(j,k \geq 1\), \[\label{eq:f32assumption} f(k^{-r}) \geq c_0 \sqrt{\frac{\log(|B_{k+j}(o)|)}{\log(|B_j(o)|)}}.\qquad{(4)}\] Then there exist \(\frac{2 \beta M_f}{c}-\)regular Gibbs measures \(\nu^{+}_{\beta, \rho}\), \(\nu^{-}_{\beta, \rho}\) such that \[\lim_{\Lambda \nearrow V}\nu_{\Lambda, \beta, \rho}^{\xi^{+}} =\nu^{+}_{\beta, \rho}, \qquad \lim_{\Lambda \nearrow V}\nu_{\Lambda, \beta, \rho}^{\xi^{-}}=\nu^{-}_{\beta, \rho}.\] Moreover, for any \(a>0\), any \(a-\)regular Gibbs measure \(\nu\) satisfies \(\nu^{-}_{\beta, \rho} \preceq \nu \preceq \nu^{+}_{\beta, \rho}\).

Proposition 13 includes the case of nearest-neighbour interactions, as \(f\) can be chosen arbitrarily in this case. Also note that if \(G\) is vertex-transitive then \(|B_{k+j}(o)|\leq |B_k(o)||B_j(o)|\) and the condition on \(f\) simplifies to \(f(k^{-r}) \geq c_0 \sqrt{\log(|B_k(o)|)}\). For the \(\varphi^4\) model, as a corollary of the Lee–Yang theorem, \(\nu^{+}_{\beta, \rho}\) coincides with the measure defined with an external field \(h\) by first taking \(\Lambda \nearrow V\) and then taking the limit as \(h \searrow 0\) (see [4]). See also [1], [10] for constructions of the plus measure when \(V = \mathbb{Z}^{d}\).

The main ingredient in the proof of Proposition 13 is the following lemma, which allows us to obtain monotonicity in \(\Lambda\) for the measures \(\nu_{\Lambda, \beta, \rho}^{\xi^{+}}\) up to an error term which tends to 0 as \(\Lambda \nearrow V\).

Lemma 7. Consider the event \(F_{\Lambda, \Lambda'} = \{|\varphi_x| \leq \xi^{+}_x \;\forall x \in \Lambda \setminus \Lambda'\}\). If \(J\) and \(f\) satisfy the assumptions of Proposition 13, then \(\nu_{\Lambda, \beta, \rho}^{\xi^{+}}[F_{\Lambda, \Lambda'}^{\mathsf{c}}] \rightarrow 0\) uniformly in \(\Lambda \supset \Lambda'\) as \(\Lambda' \nearrow V\).

Proof. We will drop \(\beta, \rho\) from the notation and just write \(\nu_{\Lambda}^{\xi}\) for the finite-volume measure on \(\Lambda\) with boundary conditions \(\xi\). Let \(\lambda = \frac{1}{c}\), where \(c\) is as in Definition 5. Applying Theorem 6 with \(a = 4 \beta M_f \lambda\), together with a union bound, yields \[\nu_{\Lambda}^{\xi^{+}}[F_{\Lambda, \Lambda'}^{\mathsf{c}}] \leq \sum_{x \in \Lambda \setminus \Lambda'} \nu_{\Lambda}^{\xi^{+}}[|\varphi_x| > \xi^{+}_x] \leq \frac{1}{\rho_{\frac{a}{2}}(\mathbb{R})} \sum_{x \in \Lambda \setminus \Lambda'} \exp(\tilde{C} A(x, \Lambda, \lambda)^2 ) \rho_{\frac{a}{2}}[|\varphi_x| > \xi^{+}_x].\] Let \(a' > 0\) be a constant to be determined. Applying Markov’s inequality to the random variable \(e^{a' \varphi_x^{2}}\), we have \[\label{eq:Markov} \nu_{\Lambda}^{\xi^{+}}[F_{\Lambda, \Lambda'}^{\mathsf{c}}] \leq \frac{\rho_{\frac{a}{2}}[e^{a' \varphi_x^2}]}{\rho_{\frac{a}{2}}(\mathbb{R})} \sum_{x \in \Lambda \setminus \Lambda'} \exp(\tilde{C} A(x, \Lambda, \lambda)^2 ) |B_{d_{G}(o, x)}(o)|^{-a'}.\tag{29}\] We will show that there exists a constant \(C' \geq 1\) such that for any finite \(\Lambda \subset V\) containing \(o\) and any \(x \in \Lambda \setminus \{o\}\), \[\label{eq:bound32on32A} A(x, \Lambda, \lambda) \leq \sqrt{C' \log(|B_{d_G(o, x)}(o)|)}.\tag{30}\] Combining 29 and 30 gives for any \(\Lambda'\) containing \(o\) \[\begin{align} \nu_{\Lambda}^{\xi^{+}}[F_{\Lambda, \Lambda'}^{\mathsf{c}}] \leq \frac{\rho_{\frac{a}{2}}[e^{a' \varphi_x^2}]}{\rho_{\frac{a}{2}}(\mathbb{R})} \sum_{x \in \Lambda \setminus \Lambda'} |B_{d_{G}(o, x)}(o)|^{\tilde{C} C' -a'}\leq \frac{\rho_{\frac{a}{2}}[e^{a' \varphi_x^2}]}{\rho_{\frac{a}{2}}(\mathbb{R})} \sum_{i = g(\Lambda')}^{\infty} |B_{i}(o)|^{1+ \tilde{C} C' - a'}, \end{align}\] where \(g(\Lambda') = \min_{x \in V \setminus \Lambda'} d_G(o, x)\). By choosing \(a'\) appropriately, the last sum converges and decreases to \(0\) as \(\Lambda' \nearrow V\).

It remains to prove 30 . Let \(C' \geq 1\) be a constant to be determined and set \[\mathcal{A}_x = \sqrt{C' \log(|B_{d_G(o, x)}(o)|)}.\] We aim to show that \(C'\) can be chosen so that for any \(\Lambda \Subset V\), \(x \in \Lambda \setminus \{o\}\) and any walk \(x_0, \ldots, x_m\) from \(x\) to a vertex \(z \in V \setminus \Lambda\), \[\begin{align} \label{eq:walk32requirement32n612} C\mathcal{A}_{x} \lambda^{m} \prod_{i = 1}^{m} f(J_{x_{i-1}, x_i}) \geq |\xi^{+}_z|, \end{align}\tag{31}\] which implies that \(A(x, \Lambda, \lambda) \leq \mathcal{A}_x\). As in the proof of Proposition 12, we can reduce the walk \(x_0, \ldots, x_m\) to a one-step walk \(x_0, x_m\) by using that \(f(J_{x_{i-1}, x_{i}}) \geq f(d_G(x_{i-1}, x_{i})^{-r})\) and applying the inequality 27 . This gives \[\begin{align} \label{eq:walk32reduction} C\mathcal{A}_{x} \lambda^{m} \prod_{i = 1}^{m} f(J_{x_{i-1}, x_i}) \geq \frac{C\sqrt{C'}}{c} \sqrt{\log(|B_{d_G(o, x)}(o)|)} f(d_G(x, z)^{-r}), \end{align}\tag{32}\] and ?? implies that \[\begin{align} \label{eq:f32ball32assumption} \frac{1}{c_0} \sqrt{\log(|B_{d_G(o, x)}(o)|)} f(d_G(x, z)^{-r}) \geq \sqrt{\log(|B_{d_{G}(o, x) + d_G(x, z)}(o)|)} \geq |\xi^{+}_z|. \end{align}\tag{33}\] Combining 32 and 33 , we see that it is possible to choose \(C'\) so that 31 is satisfied, completing the proof of 30 and of the lemma. ◻

We now proceed with the proof of Proposition 13.

Proof of Proposition 13. We only prove the statements for \(\nu^{+}_{\beta, \rho}\). As we have fixed \(\beta, \rho\) we will drop them from the notation and just write \(\nu_{\Lambda}^{\xi}\) for the finite-volume measure on \(\Lambda\) with boundary conditions \(\xi\). Let \(H\) be an increasing event that depends only on spins inside a finite subset \(\Lambda' \subset V\) and let \((\Lambda_i)_{i \geq 1}\) be a sequence of finite subsets of \(V\) with \(\Lambda_i \nearrow V\) as \(i \rightarrow \infty\). For \(k \geq i\), write \(F_{k,i}\) for the event \(F_{\Lambda_{k}, \Lambda_i}\) defined in Lemma 7. Using the domain Markov property and the fact that if \(\varphi \in F_{k,i}\), then Proposition 3 implies that \(\nu_{\Lambda_i}^{\varphi}[H] \leq \nu_{\Lambda_i}^{\xi^{+}}[H]\), we have for any \(k \geq i\) such that \(\Lambda' \subset\Lambda_i\), \(\nu_{\Lambda_{k}}^{\xi^{+}}[H] \leq \nu_{\Lambda_i}^{\xi^{+}}[H] + \nu_{\Lambda_{k}}^{\xi^{+}}[F_{k,i}^{\mathsf{c}}]\). Sending first \(k\) to infinity, and then \(i\) to infinity, and using Lemma 7, we get that \(\limsup_{k\to\infty}\nu_{\Lambda_{k}}^{\xi^{+}}[H]\leq \liminf_{i\to\infty}\nu_{\Lambda_{i}}^{\xi^{+}}[H]\). Hence \(\lim_{\Lambda \nearrow V} \nu_{\Lambda}^{\xi+}[H]\) exists for any increasing event \(H\) depending only on finitely many spins. As these events generate the \(\sigma-\)algebra, we obtain convergence of \(\nu_{\Lambda}^{\xi+}\) to a measure \(\nu^{+}\) as \(\Lambda \nearrow V\).

The assumption ?? implies that the boundary conditions \(\xi^{+}\) satisfy the assumptions of Proposition 12. Hence, ?? is satisfied with \(\lambda = \frac{1}{c}\), and we can apply Corollary 2 to deduce that \(\nu^{+}\) is an \(a\)-regular Gibbs measure for any \(a \geq 2 \beta M_f \lambda\).

Now consider any \(a>0\) and suppose \(\nu\) is an \(a-\)regular Gibbs measure. Then for any finite \(\Lambda \subset V\), the DLR equation gives that \[\begin{align} \label{eq:32xi324332DLR} \nu[H] = \nu[F_{\Lambda}] \int_{\varphi \in \mathbb{R}^{V}} \nu_{\Lambda}^{\varphi}[H] \mathrm{d} \nu(\varphi | F_{\Lambda}) + \nu[F_{\Lambda}^{\mathsf{c}}] \int_{\varphi \in \mathbb{R}^{V}} \nu_{\Lambda}^{\varphi}[H] \mathrm{d} \nu(\varphi | F_{\Lambda}^{\mathsf{c}}), \end{align}\tag{34}\] where \(F_{\Lambda} = \{\varphi:\varphi_x \leq \xi^{+}_x \, \forall x \in V\setminus \Lambda\}\). We can show that \(\nu[F_{\Lambda}^{\mathsf{c}}] \rightarrow 0\) as \(\Lambda \nearrow V\) in the same way as in the proof of Lemma 7: first using a union bound, regularity, and Markov’s inequality, we have for any \(a' > 0\) \[\nu[F_{\Lambda}^{\mathsf{c}}] \leq \sum_{x \in V \setminus \Lambda} \nu[|\varphi_x| \geq \xi^{+}_x] \leq \frac{B \rho_{a}[e^{a' \varphi_x^2}]}{\rho_{a}(\mathbb{R})} \sum_{x \in V \setminus \Lambda} |B_{d_{G}(o, x)}(o)|^{-a'}.\] It then follows that \(\nu[F_{\Lambda}^{\mathsf{c}}] \rightarrow 0\) as \(\Lambda \nearrow V\), provided that \(a'\) is chosen large enough. Hence taking \(\Lambda \nearrow V\) in 34 and using Proposition 3, we have \(\nu[H] \leq \nu^{+}[H]\). ◻

5.4 An alternative construction of the plus measure↩︎

One potential disadvantage of the construction in Proposition 13 is that it relies on growing boundary conditions, so the finite-volume measures are not regular up to the boundary. In this section, we provide a new way of constructing the infinite-volume plus measure without growing boundary conditions in the case of nearest-neighbour interactions. We start by stating the following corollary of Theorem 6, which applies for any interactions \(J\) satisfying [C1] and [C2] and is of a similar nature to [13]. Given \(a>0\) and \(B_x>0\), we define \(\zeta_x=\zeta_{x,a,B_x}\) to be a single-site measure that depends on the vertex \(x\) (see Remark 7), defined by \(\mathrm{d} \zeta_x(u) = \mathbb{1}_{\{u \geq B_x\}} \mathrm{d} \rho_{a}(u - B_x)\). Below, we let \[B_x = \left( \frac{2}{a} \left( \tilde{C} A(x, \Lambda, \xi, C)^2 + \log(\rho_{a}(\mathbb{R})) - \log(\rho_{\frac{a}{2}}(\mathbb{R}))\right) \right)^{\frac{1}{2}},\] with \(C, \tilde{C}\) the constants from Theorem 6.

Corollary 3. Let \(a \geq 4 \beta M_f\), \(\lambda \leq \frac{a}{4 \beta M_f}\), and assume that \(\rho([0, \infty)) > 0\). For any finite \(\Lambda \subset V\) and \(\Lambda' \subset \Lambda\), and any boundary conditions \(\xi\) such that \(\sum_{y \in V} |J_{x, y} \xi_y| < \infty\) for all \(x \in \Lambda\), \(\nu_{(\Lambda|\Lambda'), \beta, \rho}^{\xi}\) is stochastically dominated by \(\nu_{\Lambda', 0, \zeta}^{0}\).

Proof. We aim to show that for any \(u \in \mathbb{R}^{\Lambda'}\), \[\nu_{\Lambda, \beta, \rho}^{\xi} [\varphi_x \geq u_x, \forall x \in \Lambda'] \leq \nu_{\Lambda', 0, \rho_a}^{0} [\varphi_x + B_x \geq u_x, \forall x \in \Lambda' \mid \varphi_x \geq 0, \forall x \in \Lambda'].\] The probability on the right hand side above is equal to \(\nu_{\Lambda, 0, \zeta}^{0} [\varphi_x \geq u_x, \forall x \in \Lambda']\), so this implies the desired stochastic domination. Applying Theorem 6 with \(\Lambda_{u} := \{x \in \Lambda' : u_x \geq B_x\}\) in place of \(\Lambda'\), we obtain \[\begin{align} \nu_{\Lambda, \beta, \rho}^{\xi} [\varphi_x \geq u_x, \forall x \in \Lambda'] &\leq \nu_{\Lambda, \beta, \rho}^{\xi} [\varphi_x \geq u_x, \forall x \in \Lambda_{u}]\\ &\leq \left(\prod_{x \in \Lambda_u}\exp(\tilde{C} A(x, \Lambda)^2) \right) \nu_{\Lambda_u, 0, \rho_{\frac{a}{2}}}^{0}[\varphi_x \geq u_x, \forall x \in \Lambda_u]\\ &\leq \prod_{x \in \Lambda_u} \frac{1}{\rho_{\frac{a}{2}}(\mathbb{R})} \int_{u_x}^{\infty} \exp \left( \tilde{C} A(x, \Lambda)^2 -\frac{a}{2}|\varphi_x|^{2} \right) \mathrm{d} \rho_{a} (\varphi_x). \end{align}\] The choice of \(B_x\) gives that \(\exp\left(\tilde{C} A(x, \Lambda)^2 -\frac{a}{2}|\varphi_x|^{2} \right) \leq \frac{\rho_{\frac{a}{2}}(\mathbb{R})}{\rho_{a}(\mathbb{R})}\) whenever \(\varphi_x \geq B_x\), so since \(u_x \geq B_x\) for \(x \in \Lambda_u\), \[\begin{align} \nu_{\Lambda, \beta, \rho}^{\xi} [\varphi_x \geq u_x, \forall x \in \Lambda'] &\leq \prod_{x \in \Lambda_{u}} \frac{1}{\rho_{a}(\mathbb{R})} \int_{u_x}^{\infty} \mathrm{d} \rho_{a} (\varphi_x)\\ &\leq \nu_{\Lambda', 0, \rho_a}^{0}[\varphi_x + B_x \geq u_x, \forall x \in \Lambda' \mid \varphi_x \geq 0, \forall x \in \Lambda']. \end{align}\] ◻

We now show how the above corollary allows us to construct the plus-measure without the need for growing boundary conditions. We give two constructions, one with random boundary conditions, the other by making the single-site measure depend on the vertex. We will work on a graph \(G\) of degree bounded by some constant \(D>0\) and consider nearest-neighbour interactions on \(G\).

Denote by \(\partial \Lambda\) the set of vertices in \(\Lambda\) that are adjacent to \(V \setminus \Lambda\). Let \(a = 8 \beta D\) and write \(B= \left( \frac{2}{a} \left( 2\tilde{C} + \log(\rho_{a}(\mathbb{R})) - \log(\rho_{\frac{a}{2}}(\mathbb{R}))\right) \right)^{\frac{1}{2}}\), where \(\tilde{C}\) is the constant given by Theorem 6. Recall the definition of the measure \(\zeta=\zeta_{a,B}\). Let us introduce the measure \(\tilde{\nu}^0_{\Lambda,\beta,\rho}\) defined on any bounded measurable function \(g: \mathbb{R}^{\Lambda \setminus \partial \Lambda} \rightarrow \mathbb{R}\) as \[\tilde{\nu}^0_{\Lambda,\beta,\rho}[g] = \int_{\xi \in \mathbb{R}^{\partial \Lambda}} \langle g\rangle_{\Lambda \setminus \partial \Lambda, \beta, \rho}^{\xi} \mathrm{d} \nu_{\partial \Lambda, 0, \zeta}^{0}(\xi).\] In words, \(\tilde{\nu}^0_{\Lambda,\beta,\rho}\) is a measure with random boundary conditions sampled from the product measure \(\nu_{\partial \Lambda, 0, \zeta}^{0}\).

Proposition 14. Let \(G=(V,E)\) be a connected graph of degree bounded by \(D>0\). Consider nearest-neighbour interactions on \(G\) and let \(\rho\) be an even measure. For every \(\beta\geq 0\), \[\tilde{\nu}^0_{\Lambda,\beta,\rho}\rightarrow \nu^{+}_{\beta, \rho} \text{ as } \Lambda \nearrow V.\] Furthermore, for every \(\beta\geq 0\) there exist \(a',B'>0\) that depend continuously on \(\beta\) such that for every \(\Lambda\Subset V\), \(\tilde{\nu}^0_{\Lambda,\beta,\rho}\) is stochastically dominated by \(\nu^0_{\Lambda,0,\zeta_{a',B'}}\).

For our second construction, we define a single-site measure \(\tilde{\rho}_{x, \Lambda}\) by \[\mathrm{d}\tilde{\rho}_{x, \Lambda}(u) = \begin{cases} \mathrm{d} \zeta_{a,B}(u) & \text{if } x\in \partial \Lambda,\\ \mathrm{d} \rho(u) & \text{otherwise.} \end{cases}\]

Proposition 15. Let \(G=(V,E)\) be a connected graph of degree bounded by \(D>0\). Consider nearest-neighbour interactions on \(G\) and let \(\rho\) be an even measure. For every \(\beta\geq 0\), \[\nu_{\Lambda, \beta, \tilde{\rho}}^{0} \rightarrow \nu^{+}_{\beta, \rho} \text{ as } \Lambda \nearrow V.\] Furthermore, for every \(\beta\geq 0\) there exist \(a',B'>0\) that depend continuously on \(\beta\) such that for every \(\Lambda\Subset V\), \(\nu^0_{\Lambda,\beta,\tilde{\rho}}\) is stochastically dominated by \(\nu^0_{\Lambda,0,\zeta_{a',B'}}\).

To prove Proposition 15, we will need to use monotonicity in \(\beta\) of the measures \(\nu_{(\Lambda | \partial \Lambda), \beta, \tilde{\rho}}^{0}\), which is provided by the following lemma.

Lemma 8. If \(\rho\) is an even measure, then for any \(\beta' \geq \beta \geq 0\) and any \(\Lambda \Subset V\), \[\nu_{(\Lambda | \partial \Lambda), \beta, \tilde{\rho}}^{0} \preceq \nu_{(\Lambda | \partial \Lambda), \beta', \tilde{\rho}}^{0}.\]

Proof. Let \(A\) be an increasing event depending only on vertices in \(\partial \Lambda\). Without loss of generality, assume that \(\nu_{(\Lambda | \partial \Lambda), \beta, \tilde{\rho}}^{0}[A] > 0\). Differentiating with respect to \(\beta\) we obtain \[\frac{\mathrm{d} \nu_{(\Lambda | \partial \Lambda), \beta, \tilde{\rho}}^{0}[A]}{\mathrm{d} \beta} = \sum_{xy \in E} \langle \mathbb{1}_{A} \varphi_x \varphi_y \rangle_{\Lambda, \beta, \tilde{\rho}}^{0} - \langle \mathbb{1}_{A} \rangle_{\Lambda, \beta, \tilde{\rho}}^{0} \langle \varphi_x \varphi_y \rangle_{\Lambda, \beta, \tilde{\rho}}^{0},\] so it suffices to show that \(\langle \varphi_x \varphi_y \mid A \rangle_{\Lambda, \beta, \tilde{\rho}}^{0} - \langle \varphi_x \varphi_y \rangle_{\Lambda, \beta, \tilde{\rho}}^{0} \geq 0\) for all \(xy \in E\).

If \(x, y \in \partial \Lambda\) then \(\varphi_x, \varphi_y \geq 0\), so \(\varphi_x\varphi_y\) is an increasing function and the desired inequality follows from the FKG inequality. Now suppose that \(x, y \in \Lambda \setminus \partial \Lambda\). We use the domain Markov property and the fact that \(\tilde{\rho} = \rho\) on \(\Lambda \setminus \partial \Lambda\) to get \[\langle \varphi_x \varphi_y \mid A \rangle_{\Lambda, \beta, \tilde{\rho}}^{0} = \int_{\eta \in (\mathbb{R}^{+})^{\partial \Lambda}} \langle \varphi_x \varphi_y \rangle_{\Lambda \setminus \partial \Lambda, \beta, \rho}^{\eta} \mathrm{d} \nu_{(\Lambda | \partial \Lambda), \beta, \tilde{\rho}}^{0} [\eta \mid A].\] Since \(\nu_{(\Lambda | \partial \Lambda), \beta, \tilde{\rho}}^{0} [\;\cdot \mid A] \succeq \nu_{(\Lambda | \partial \Lambda), \beta, \tilde{\rho}}^{0} [\;\cdot \;]\) by the FKG inequality, and \(\langle \varphi_x \varphi_y \rangle_{\Lambda \setminus \partial \Lambda, \beta, \rho}^{\eta}\) is an increasing function of \(\eta\) (which follows by differentiating and using Griffiths’ inequality), the right hand side above is at least \(\langle \varphi_x \varphi_y \rangle_{\Lambda, \beta, \tilde{\rho}}^{0}\).

It remains to consider the case when the edge \(xy\) has one endpoint in \(\partial \Lambda\) and the other endpoint in \(\Lambda \setminus \partial \Lambda\). If \(x \in \Lambda \setminus \partial \Lambda\) and \(y \in \partial \Lambda\), then \[\langle \varphi_x \varphi_y \mid A \rangle_{\Lambda, \beta, \tilde{\rho}}^{0} = \int_{\eta \in (\mathbb{R}^{+})^{\partial \Lambda}} \eta_y \langle \varphi_x \rangle_{\Lambda \setminus \partial \Lambda, \beta, \rho}^{\eta} \mathrm{d} \nu_{(\Lambda | \partial \Lambda), \beta, \tilde{\rho}}^{0} [\eta \mid A].\] Proposition 3 together with the fact that the boundary conditions \(\eta\) are positive and \(\rho\) is an even measure implies that \(\eta_y \langle \varphi_x \rangle_{\Lambda \setminus \partial \Lambda, \beta, \rho}^{\eta}\) is an increasing function of \(\eta\), so the right hand side is again at least \(\langle \varphi_x \varphi_y \rangle_{\Lambda, \beta, \tilde{\rho}}^{0}\). ◻

As a corollary, we obtain the following stochastic domination.

Corollary 4. For any \(\Lambda \Subset V\), \(\beta \geq 0\) and any even single-site measure \(\rho\), \[\tilde{\nu}^0_{\Lambda,\beta,\rho} \preceq \nu^0_{\Lambda,\beta,\tilde{\rho}}.\]

Proof. By Lemma 8, we have \(\tilde{\nu}_{(\Lambda | \partial \Lambda), 0, \rho}^{0} = \nu_{(\Lambda | \partial \Lambda), 0, \tilde{\rho}}^{0} \preceq \nu_{(\Lambda | \partial \Lambda), \beta, \tilde{\rho}}^{0}\), and stochastic domination in the whole of \(\Lambda\) follows from the domain Markov property and monotonicity in boundary conditions. ◻

In the next proposition, we show that \(\tilde{\nu}^0_{\Lambda,\beta,\rho}\) and \(\nu_{\Lambda, \beta, \tilde{\rho}}^{0}\) satisfy a form of monotonicity in the volume, which we believe to be of independent interest.

Proposition 16. Let \(G=(V,E)\) be a graph of bounded degree. For every \(\beta>0\) there exists \(r>0\) such that the following holds. Consider \(\Lambda'\subset \Lambda \Subset V\) such that \(d_G(\partial \Lambda, \Lambda')>r\). Then \(\tilde{\nu}^0_{\Lambda',\beta,\rho}\) stochastically dominates \(\nu^0_{(\Lambda | \Lambda'),\beta, \tilde{\rho}}\). In particular, we have \(\tilde{\nu}^0_{\Lambda',\beta,\rho} \succeq \tilde{\nu}^0_{(\Lambda | \Lambda'),\beta,\rho}\) and \(\nu^0_{\Lambda',\beta,\tilde{\rho}} \succeq \nu^0_{(\Lambda | \Lambda'),\beta,\tilde{\rho}}\).

Proof. Let \(\xi \sim \nu_{(\Lambda | \partial \Lambda), \beta, \tilde{\rho}}^{0}\), write \(R=\Lambda\setminus\partial\Lambda\) and consider a set \(S\subset \partial \Lambda'\). By Theorem 6, \[\mathrm{d} \nu_{R, \beta, \rho}^{\xi}[\varphi|_{S} = \psi] \leq \prod_{x \in S} e^{\tilde{C} A(x, R, \xi, C)^2} \mathrm{d} \nu_{S, 0, \rho_{\frac{a}{2}}}^{0} [\psi].\] It suffices to prove that \[\label{eq:expected32regularity} \nu_{(\Lambda | \partial \Lambda), \beta, \tilde{\rho}}^{0}\left[\prod_{x \in S} e^{\tilde{C} A(x, R, \xi, C)^2}\right]\leq e^{2\tilde{C} |S|}.\tag{35}\] Indeed, since \(S\) is an arbitrary subset of \(\partial \Lambda'\), 35 implies that \(\nu^0_{(\Lambda | \partial \Lambda'),\beta,\tilde{\rho}}\) is a (finite-volume) \(a/2\)-regular measure with constant \(B=2\tilde{C}\), and we can apply the argument of Corollary 3 to deduce that \(\nu_{\partial \Lambda', 0, \zeta}^{0} =\tilde{\nu}^0_{(\Lambda' | \partial \Lambda'),\beta,\rho}\) stochastically dominates \(\nu^0_{(\Lambda | \partial \Lambda'),\beta,\tilde{\rho}}\). Then the desired stochastic domination in the whole of \(\Lambda'\) follows from monotonicity in boundary conditions. By corollary 4, we also get \(\tilde{\nu}^0_{\Lambda',\beta,\rho} \succeq \tilde{\nu}^0_{(\Lambda | \Lambda'),\beta,\rho}\) and \(\nu^0_{\Lambda',\beta,\tilde{\rho}} \succeq \nu^0_{(\Lambda | \Lambda'),\beta,\tilde{\rho}}\).

Let us now prove 35 . Note that \[A(x, R, \xi, C)^2\leq\max \left\{ 1, \max_{z \in \partial \Lambda} \left(\frac{|\xi_z|^2}{C^2\lambda^{2d_{\Lambda}(x, z)}}\right) \right\}\leq 1+\sum_{z \in \partial \Lambda} \frac{|\xi_z|^2}{C^2\lambda^{2d_{\Lambda}(x, z)}}.\] Hence \[\label{eq:32sum32of32A32bound} \sum_{x\in S} A(x, R, \xi, C)^2\leq |S|+\sum_{z\in \partial \Lambda} \frac{|\xi_z|^2}{C^2}\sum_{k\geq d_{\Lambda}(z,S)}\frac{|B_k(z)|}{\lambda^{2k}} \leq |S|+\sum_{z\in \partial \Lambda} \frac{|\xi_z|^2}{\lambda^{d_{\Lambda}(z,S)}},\tag{36}\] provided \(\lambda\geq 2D\), where \(D\) is the maximum degree, and \(d_G(\partial \Lambda, \Lambda')\) is large enough. Now let \(B' > 0\) and let \(\zeta'\) be the single-site measure given by \(\mathrm{d} \zeta'(u) = \mathbb{1}_{\{u \geq B'\}} e^{a |u - B'|^2} \mathrm{d} \zeta(u - B')\). By Corollary 3, we have \(\nu_{(\Lambda | \partial \Lambda), \beta, \tilde{\rho}}^{0} \preceq \nu^0_{\partial \Lambda, 0, \zeta'}\) for some choice of \(B'\). Therefore, using that \(\prod_{x \in S} e^{\tilde{C} A(x, R, \xi, C)^2}\) is an increasing function of \(\xi\) for \(\xi \geq 0\), we obtain \[\nu_{(\Lambda | \partial \Lambda), \beta, \tilde{\rho}}^{0}\left[\prod_{x \in S} e^{\tilde{C} A(x, R, \xi, C)^2}\right]\leq \nu_{\partial \Lambda, 0, \zeta'}^{0}\left[\prod_{x \in S} e^{\tilde{C} A(x, R, \xi, C)^2}\right]\leq e^{\tilde{C} |S|}\exp\left(C'\sum_{z\in \partial \Lambda}\lambda^{-d_{\Lambda}(z,S)}\right)\] for some constant \(C'>0\), where in the second inequality we used 36 , independence, and the inequality \(\mathbb{E}(e^{tX})\leq 1+t\mathbb{E}(e^X)\leq e^{t\mathbb{E}(e^X)}\) for any \(t\in (0,1)\) and any random variable \(X\geq 0\). By decomposing according to the points in \(S\) that attain \(d_{\Lambda}(z,S)\) we get that \[\sum_{z\in \partial \Lambda}\lambda^{-d_{\Lambda}(z,S)}\leq \sum_{x\in S} \sum_{k\geq d_G(\partial \Lambda,\Lambda')} |B_k(x)|\lambda^{-k}\leq \tilde{C}|S|/C',\] provided that \(d_{G}(\partial \Lambda,\Lambda')\) is large enough. This implies 35 and concludes the proof. ◻

We now prove convergence of the measures \(\nu_{\Lambda, \beta, \tilde{\rho}}^{0}\) and \(\tilde{\nu}^0_{\Lambda,\beta,\rho}\) to the plus measure.

Proof of Proposition 15. First note that the single-site measures \(\tilde{\rho}_{x, \Lambda}\) satisfy the assumptions of Remark 7 with \(a_{\min} = \frac{a}{2}\), and that the result of Theorem 6 still applies in this case. Therefore, there exists \(\tilde{C}_2 > 0\) such that for all \(\Lambda \Subset V\), \(\Lambda' \subset \Lambda \setminus \partial \Lambda\) and \(\psi \in \mathbb{R}^{\Lambda'}\), \[\label{eq:regularity32for32rho32tilde32n612} \mathrm{d} \nu_{\Lambda, \beta, \tilde{\rho}}^{0}[\varphi|_{\Lambda'} = \psi] \leq e^{\tilde{C}_2 |\Lambda'|} \mathrm{d} \nu_{\Lambda', 0, \rho_{\frac{a}{2}}}^{0} [\psi].\tag{37}\] By the monotonicity in volume of Proposition 16, \(\nu_{\Lambda, \beta, \tilde{\rho}}^{0}\) converges to some measure \(\tilde{\nu}\) as \(\Lambda \nearrow V\). The measure \(\tilde{\nu}\) is \(\frac{a}{2}\)-regular by 37 and is a Gibbs measure by the domain Markov property; hence \(\tilde{\nu} \preceq \nu^{+}_{\beta, \rho}\) by Proposition 13. It remains to prove that \(\nu^{+}_{\beta, \rho} \preceq \tilde{\nu}\), which implies that \(\tilde{\nu}=\nu^{+}_{\beta, \rho}\).

Let \((\Lambda_i)_{i \geq 1}\) be a sequence of finite subsets of \(V\) with \(\Lambda_i \nearrow V\) as \(i \rightarrow \infty\). Setting \(\lambda = 2\) and using 22 , we see that for each \(i \geq 1\) we can find \(k(i) \geq i\) such that \(A(x, \Lambda_{k(i)}, \xi^{+}, C) = 1\) for any \(x \in \Lambda_i\). Now using Corollary 3 and Lemma 8, \[\nu_{(\Lambda_{k(i)}| \partial \Lambda_i), \beta, \rho}^{\xi^{+}} \preceq \nu_{\partial \Lambda_i, 0, \tilde{\rho}}^{0} \preceq \nu_{(\Lambda_i|\partial \Lambda_i), \beta, \tilde{\rho}}^{0}.\] Let \(\Lambda' \Subset V\) and consider an increasing event \(H\) that depends only on spins inside \(\Lambda'\). The domain Markov property and Proposition 3 together with the above stochastic domination imply that whenever \(i\) is large enough that \(\Lambda' \subset \Lambda_i \setminus \partial \Lambda_i\), \[\begin{align} \nu_{\Lambda_{k(i)}, \beta, \rho}^{\xi^{+}} [H] &= \int_{\mathbb{R}^{\partial \Lambda_i}} \nu_{\Lambda_i \setminus \partial \Lambda_i, \beta, \rho}^{\eta}[H] \mathrm{d} \nu_{(\Lambda_{k(i)}| \partial \Lambda_i), \beta, \rho}^{\xi^{+}}[\eta]\\ &\leq \int_{\mathbb{R}^{\partial \Lambda_i}} \nu_{\Lambda_i \setminus \partial \Lambda_i, \beta, \rho}^{\eta}[H] \mathrm{d} \nu_{(\Lambda_{i}|\partial \Lambda_i), \beta, \tilde{\rho}}^{0}[\eta] = \nu_{\Lambda_i, \beta, \tilde{\rho}}^{0}[H]. \end{align}\] Taking \(i \rightarrow \infty\), we have \(\nu^{+}_{\beta, \rho}[H] \leq \tilde{\nu}[H]\).

The desired stochastic domination follows from Corollary 3. ◻

Proof of Proposition 14. First observe that the monotonicity in volume of Proposition 16 implies convergence of the measures \(\tilde{\nu}^0_{\Lambda,\beta,\rho}\) to an infinite-volume limit \(\tilde{\nu}\) as \(\Lambda \nearrow V\). By Corollary 4, we have that \(\tilde{\nu}^0_{\Lambda,\beta,\rho} \preceq \nu^0_{\Lambda,\beta,\tilde{\rho}}\) for any \(\Lambda \Subset V\), so \(\tilde{\nu} \preceq \nu^{+}_{\beta, \rho}\) because \(\nu^0_{\Lambda,\beta,\tilde{\rho}} \rightarrow \nu^{+}_{\beta, \rho}\) by Proposition 15. The proof that \(\nu^{+}_{\beta, \rho} \preceq \tilde{\nu}\) is similar to that of Proposition 15, and in fact, even simpler, as one does not need to use Lemma 8. ◻

References↩︎

[1]
J. L. Lebowitz and E. Presutti, “Statistical mechanics of systems of unbounded spins,” Communications in Mathematical Physics, vol. 50, no. 3, pp. 195–218, 1976.
[2]
D. Ruelle, “Superstable interactions in classical statistical mechanics,” Communications in Mathematical Physics, vol. 18, no. 2, pp. 127–159, 1970.
[3]
D. Ruelle, “Probability estimates for continuous spin systems,” Communications in Mathematical Physics, vol. 50, no. 3, pp. 189–194, 1976.
[4]
T. S. Gunaratnam, C. Panagiotis, R. Panis, and F. Severo, Available at https://arxiv.org/abs/2211.00319“Random tangled currents for \(\varphi^{4}\): Translation invariant Gibbs measures and continuity of the phase transition,” Journal of the European Mathematical Society (to appear), 2025.
[5]
H. Duminil-Copin, Available at https://arxiv.org/abs/1707.00520“Lectures on the Ising and Potts models on the hypercubic lattice,” in PIMS-CRM summer school in probability, Springer, 2017, pp. 35–161.
[6]
S. Friedli and Y. Velenik, Statistical Mechanics of Lattice Systems: A Concrete Mathematical Introduction. Cambridge University Press, 2017.
[7]
J. Glimm and A. Jaffe, Quantum physics : A functional integral point of view, 2nd ed. Springer New York, 1987.
[8]
W. Werner and E. Powell, Lecture notes on the gaussian free field, vol. 28. Paris: Société Mathématique de France, 2021.
[9]
M. Cassandro, E. Olivieri, A. Pellegrinotti, and E. Presutti, Existence and uniqueness of DLR measures for unbounded spin systems,” Zeitschrift für Wahrscheinlichkeitstheorie und verwandte Gebiete, vol. 41, no. 4, pp. 313–334, 1978.
[10]
J. Bellissard and R. Høegh-Krohn, “Compactness and the maximal Gibbs state for random Gibbs fields on a lattice,” Communications in Mathematical Physics, vol. 84, no. 3, pp. 297–327, 1982.
[11]
S. Albeverio, Y. G. Kondratiev, M. Röckner, and T. V. Tsikalenko, A priori estimates for symmetrizing measures and their applications to Gibbs states,” Journal of Functional Analysis, vol. 171, no. 2, pp. 366–400, 2000.
[12]
A. Raoufi, “Translation-invariant Gibbs states of the Ising model: General setting,” The Annals of Probability, vol. 48, no. 2, pp. 760–777, 2020.
[13]
T. S. Gunaratnam, C. Panagiotis, R. Panis, and F. Severo, Available at https://arxiv.org/abs/2501.05353“The supercritical phase of the \(\varphi^4\) model is well behaved,” Preprint, 2025.
[14]
R. van der Hofstad, Random graphs and complex networks. Volume 1, vol. 43. Cambridge University Press, 2017.