Searcharxiv⌕ Search

arXiv subjects

Jason Miller

Publications and source records attributed to Jason Miller.

90 records · Page 5Linked to original sources

Gaussian free field light cones and SLE$_κ(ρ)$

We derive a surprising correspondence between SLE$_κ(ρ)$ processes and light cones of the Gaussian free field (GFF). Recall that (one-sided, chordal, origin-seeded) SLE$_κ(ρ)$ processes are in some sense the simplest and most natural variants of the Schramm-Loewner evolution. They were originally defined only for $ρ> -2$, but one can use Lévy compensation to extend the definition to any $ρ> -2-\tfracκ{2}$ and to obtain qualitatively different curves. The triangle $T = \{(κ, ρ): (-2-\tfracκ{2})\vee (\tfracκ{2}-4) < ρ< -2 \}$ is the primary focus of this paper. When $(κ, ρ) \in T$, the SLE$_κ(ρ)$ curves are highly non-simple (and double points are dense) even though $κ< 4$. Let $h$ be an instance of the GFF. Fix $κ\in (0,4)$ and $χ= 2/\sqrtκ - \sqrtκ/2$. Recall that an imaginary geometry ray is a flow line of $e^{i(h/χ+θ)}$ that looks locally like SLE$_κ$. The light cone with parameter $θ\in [0, π]$ is the set of points reachable from the origin by a sequence of rays with angles in $[-θ/2, θ/2]$. When $θ=0$, the light cone looks like SLE$_κ$, and when $θ= π$ it looks like the range of an SLE$_{16/κ}$. We find that when $θ\in (0, π)$ the light cones are either fractal carpets with a dense set of holes or space-filling regions with no holes. We show that every non-space-filling light cone (with $θ\in (0,π]$ and $κ\in (0,4)$) agrees in law with the range of an SLE$_κ(ρ)$ process with $(κ, ρ) \in T$. Conversely, the range of any SLE$_κ(ρ)$ with $(κ,ρ) \in T$ agrees in law with a non-space-filling light cone. As a consequence, we obtain the first proof that these SLE$_κ(ρ)$ processes are continuous and show that they are natural path-valued functions of the GFF.

math.PR↗

Extreme nesting in the conformal loop ensemble

The conformal loop ensemble $\operatorname {CLE}_κ$ with parameter $8/3<κ<8$ is the canonical conformally invariant measure on countably infinite collections of noncrossing loops in a simply connected domain. Given $κ$ and $ν$, we compute the almost-sure Hausdorff dimension of the set of points $z$ for which the number of CLE loops surrounding the disk of radius $\varepsilon$ centered at $z$ has asymptotic growth $ν\log (1/\varepsilon )$ as $\varepsilon \to0$. By extending these results to a setting in which the loops are given i.i.d. weights, we give a CLE-based treatment of the extremes of the Gaussian free field.

math.PR↗

Imaginary Geometry I: Interacting SLEs

Fix constants χ>0 and θ\in [0,2π), and let h be an instance of the Gaussian free field on a planar domain. We study flow lines of the vector field e^{i(h/χ+θ)} starting at a fixed boundary point of the domain. Considering all θ\in [0,2π), one obtains a family of curves that look locally like SLE_κ, with κ\in (0,4), where χ= 2/κ^{1/2} - κ^{1/2}/2, which we interpret as the rays of a random geometry with purely imaginary curvature. We extend the fundamental existence and uniqueness results about these paths to the case that the paths intersect the boundary. We also show that flow lines of different angles cross each other at most once but (in contrast to what happens when h is smooth) may bounce off of each other after crossing. Flow lines of the same angle started at different points merge into each other upon intersecting, forming a tree structure. We construct so-called counterflow lines (SLE_{16/κ}) within the same geometry using ordered "light cones" of points accessible by angle-restricted trajectories and develop a robust theory of flow and counterflow line interaction. The theory leads to new results about SLE. For example, we prove that SLE_κ(ρ) processes are almost surely continuous random curves, even when they intersect the boundary, and establish Duplantier duality for general SLE_{16/κ}(ρ) processes.

math.PR↗

Imaginary geometry II: reversibility of SLE_κ(ρ_1;ρ_2) for κ\in (0,4)

Given a simply connected planar domain D, distinct points x,y \in \partial D, and κ>0, the Schramm-Loewner evolution SLE_κis a random continuous non-self-crossing path in the closure of D from x to y. The SLE_κ(ρ_1;ρ_2) processes, defined for ρ_1, ρ_2 > -2, are in some sense the most natural generalizations of SLE_κ. When κ\leq 4, we prove that the law of the time-reversal of an \SLE_κ(ρ_1;ρ_2) from x to y is, up to parameterization, an SLE_κ(ρ_2;ρ_1) from y to x. This assumes that the "force points" used to define SLE_κ(ρ_1;ρ_2) are immediately to the left and right of the SLE seed. A generalization to arbitrary (and arbitrarily many) force points applies whenever the path does not (or is conditioned not to) hit the boundary of D except at the endpoints. The time-reversal symmetry has a particularly natural interpretation when the paths are coupled with the Gaussian free field and viewed as rays of a random geometry. It allows us to couple two instances of the Gaussian free field (with different boundary conditions) so that their difference is almost surely constant on either side of the path. In a fairly general sense, adding appropriate constants to the two sides of a ray reverses its orientation.

math.PR↗

Imaginary geometry III: reversibility of SLE_κ for κ\in (4,8)

Suppose that D is a planar Jordan domain and x and y are distinct boundary points of D. Fix κ\in (4,8) and let η be an SLE_κprocess from x to y in D. We prove that the law of the time-reversal of ηis, up to reparameterization, an SLE_κprocess from y to x in D. More generally, we prove that SLE_κ(ρ_1;ρ_2) processes are reversible if and only if both ρ_i are at least κ/2-4, which is the critical threshold at or below which such curves are boundary filling. Our result supplies the missing ingredient needed to show that for all κ\in (4,8) the so-called conformal loop ensembles CLE_κ are canonically defined, with almost surely continuous loops. It also provides an interesting way to couple two Gaussian free fields (with different boundary conditions) so that their difference is piecewise constant and the boundaries between the constant regions are SLE_κcurves.

math.PR↗

Brownian motion correlation in the peanosphere for $κ> 8$

The peanosphere (or "mating of trees") construction of Duplantier, Miller, and Sheffield encodes certain types of $γ$-Liouville quantum gravity (LQG) surfaces ($γ\in (0,2)$) decorated with an independent SLE$_κ$ ($κ= 16/γ^2 > 4$) in terms of a correlated two-dimensional Brownian motion and provides a framework for showing that random planar maps decorated with statistical physics models converge to LQG decorated with an SLE. Previously, the correlation for the Brownian motion was only explicitly identified as $-\cos(4π/κ)$ for $κ\in (4,8]$ and unknown for $κ> 8$. The main result of this work is that this formula holds for all $κ> 4$. This supplies the missing ingredient for proving convergence results of the aforementioned type for $κ> 8$. Our proof is based on the calculation of a certain tail exponent for SLE$_κ$ on a quantum wedge and then matching it with an exponent which is well-known for Brownian motion.

math.PR↗

The conformal loop ensemble nesting field

The conformal loop ensemble CLE$_κ$ with parameter $8/3 < κ< 8$ is the canonical conformally invariant measure on countably infinite collections of non-crossing loops in a simply connected domain. We show that the number of loops surrounding an $\varepsilon$-ball (a random function of $z$ and $\varepsilon$) minus its expectation converges almost surely as $\varepsilon\to 0$ to a random conformally invariant limit in the space of distributions, which we call the nesting field. We generalize this result by assigning i.i.d. weights to the loops, and we treat an alternate notion of convergence to the nesting field in the case where the weight distribution has mean zero. We also establish estimates for moments of the number of CLE loops surrounding two given points.

math.PR↗

The Hausdorff dimension of the CLE gasket

The conformal loop ensemble $\mathrm{CLE}_κ$ is the canonical conformally invariant probability measure on noncrossing loops in a proper simply connected domain in the complex plane. The parameter $κ$ varies between $8/3$ and $8$; $\mathrm{CLE}_{8/3}$ is empty while $\mathrm {CLE}_8$ is a single space-filling loop. In this work, we study the geometry of the $\mathrm{CLE}$ gasket, the set of points not surrounded by any loop of the $\mathrm{CLE}$. We show that the almost sure Hausdorff dimension of the gasket is bounded from below by $2-(8-κ)(3κ-8)/(32κ)$ when $4<κ<8$. Together with the work of Schramm-Sheffield-Wilson [Comm. Math. Phys. 288 (2009) 43-53] giving the upper bound for all $κ$ and the work of Nacu-Werner [J. Lond. Math. Soc. (2) 83 (2011) 789-809] giving the matching lower bound for $κ\le4$, this completes the determination of the $\mathrm{CLE}_κ$ gasket dimension for all values of $κ$ for which it is defined. The dimension agrees with the prediction of Duplantier-Saleur [Phys. Rev. Lett. 63 (1989) 2536-2537] for the FK gasket.

math.PR↗

Quantum Loewner Evolution

What is the scaling limit of diffusion limited aggregation (DLA) in the plane? This is an old and famously difficult question. One can generalize the question in two ways: first, one may consider the {\em dielectric breakdown model} $η$-DBM, a generalization of DLA in which particle locations are sampled from the $η$-th power of harmonic measure, instead of harmonic measure itself. Second, instead of restricting attention to deterministic lattices, one may consider $η$-DBM on random graphs known or believed to converge in law to a Liouville quantum gravity (LQG) surface with parameter $γ\in [0,2]$. In this generality, we propose a scaling limit candidate called quantum Loewner evolution, QLE$(γ^2, η)$. QLE is defined in terms of the radial Loewner equation like radial SLE, except that it is driven by a measure valued diffusion $ν_t$ derived from LQG rather than a multiple of a standard Brownian motion. We formalize the dynamics of $ν_t$ using an SPDE. For each $γ\in (0,2]$, there are two or three special values of $η$ for which we establish the existence of a solution to these dynamics and explicitly describe the stationary law of $ν_t$. We also explain discrete versions of our construction that relate DLA to loop-erased random walk and the Eden model to percolation. A certain "reshuffling" trick (in which concentric annular regions are rotated randomly, like slot machine reels) facilitates explicit calculation. We propose QLE$(2,1)$ as a scaling limit for DLA on a random spanning-tree-decorated planar map, and QLE$(8/3,0)$ as a scaling limit for the Eden model on a random triangulation. We propose using QLE$(8/3,0)$ to endow pure LQG with a distance function, by interpreting the region explored by a branching variant of QLE$(8/3,0)$, up to a fixed time, as a metric ball in a random metric space.

math.PR↗

Uniformity of the late points of random walk on Z_n^d for d >= 3

Suppose that $X$ is a simple random walk on $\Z_n^d$ for $d \geq 3$ and, for each $t$, we let $\U(t)$ consist of those $x \in \Z_n^d$ which have not been visited by $X$ by time $t$. Let $\tcov$ be the expected amount of time that it takes for $X$ to visit every site of $\Z_n^d$. We show that there exists $0 < α_0(d) \leq α_1(d) < 1$ and a time $t_* = \tcov(1+o(1))$ as $n \to \infty$ such that the following is true. For $α> α_1(d)$ (resp.\ $α< α_0(d)$), the total variation distance between the law of $\U(αt_*)$ and the law of i.i.d.\ Bernoulli random variables indexed by $\Z_n^d$ with success probability~$n^{-αd}$ tends to~$0$ (resp.\ $1$) as $n \to \infty$. Let $τ_α$ be the first time $t$ that $|\U(t)| = n^{d-αd}$. We also show that the total variation distance between the law of $\U(τ_α)$ and the law of a uniformly chosen set from $\Z_n^d$ with size $n^{d-αd}$ tends to $0$ (resp.\ $1$) for $α> α_1(d)$ (resp.\ $α< α_0(d)$) as $n \to \infty$.

math.PR↗

Intersections of SLE Paths: the double and cut point dimension of SLE

We compute the almost-sure Hausdorff dimension of the double points of chordal SLE_kappa for kappa > 4, confirming a prediction of Duplantier-Saleur (1989) for the contours of the FK model. We also compute the dimension of the cut points of chordal SLE_kappa for kappa > 4 as well as analogous dimensions for the radial and whole-plane SLE_kappa(rho) processes for kappa > 0. We derive these facts as consequences of a more general result in which we compute the dimension of the intersection of two flow lines of the formal vector field e^{ih/chi}, where h is a Gaussian free field and chi > 0, of different angles with each other and with the domain boundary.

math.PR↗

Painting a graph with competing random walks

Let $X_1,X_2$ be independent random walks on $\mathbf{Z}_n^d$, $d\geq3$, each starting from the uniform distribution. Initially, each site of $\mathbf{Z}_n^d$ is unmarked, and, whenever $X_i$ visits such a site, it is set irreversibly to $i$. The mean of $|\mathcal{A}_i|$, the cardinality of the set $\mathcal{A}_i$ of sites painted by $i$, once all of $\mathbf{Z}_n^d$ has been visited, is $\frac{1}{2}n^d$ by symmetry. We prove the following conjecture due to Pemantle and Peres: for each $d\geq3$ there exists a constant $α_d$ such that $\lim_{n\to\infty}\operatorname{Var}(|\mathcal {A}_i|)/h_d(n)=\frac{1}{4}α_d$ where $h_3(n)=n^4$, $h_4(n)=n^4(\log n)$ and $h_d(n)=n^d$ for $d\geq5$. We will also identify $α_d$ explicitly and show that $α_d\to1$ as $d\to\infty$. This is a special case of a more general theorem which gives the asymptotics of $\operatorname{Var}(|\mathcal{A}_i|)$ for a large class of transient, vertex transitive graphs; other examples include the hypercube and the Caley graph of the symmetric group generated by transpositions.

math.PR↗

Uniform mixing time for Random Walk on Lamplighter Graphs

Suppose that $\CG$ is a finite, connected graph and $X$ is a lazy random walk on $\CG$. The lamplighter chain $X^\diamond$ associated with $X$ is the random walk on the wreath product $\CG^\diamond = \Z_2 \wr \CG$, the graph whose vertices consist of pairs $(f,x)$ where $f$ is a labeling of the vertices of $\CG$ by elements of $\Z_2$ and $x$ is a vertex in $\CG$. There is an edge between $(f,x)$ and $(g,y)$ in $\CG^\diamond$ if and only if $x$ is adjacent to $y$ in $\CG$ and $f(z) = g(z)$ for all $z \neq x,y$. In each step, $X^\diamond$ moves from a configuration $(f,x)$ by updating $x$ to $y$ using the transition rule of $X$ and then sampling both $f(x)$ and $f(y)$ according to the uniform distribution on $\Z_2$; $f(z)$ for $z \neq x,y$ remains unchanged. We give matching upper and lower bounds on the uniform mixing time of $X^\diamond$ provided $\CG$ satisfies mild hypotheses. In particular, when $\CG$ is the hypercube $\Z_2^d$, we show that the uniform mixing time of $X^\diamond$ is $Θ(d 2^d)$. More generally, we show that when $\CG$ is a torus $\Z_n^d$ for $d \geq 3$, the uniform mixing time of $X^\diamond$ is $Θ(d n^d)$ uniformly in $n$ and $d$. A critical ingredient for our proof is a concentration estimate for the local time of random walk in a subset of vertices.

math.PR↗

Uniformity of the uncovered set of random walk and cutoff for lamplighter chains

We show that the measure on markings of $\mathbf {Z}_n^d$, $d\geq3$, with elements of ${0,1}$ given by i.i.d. fair coin flips on the range $\mathcal {R}$ of a random walk $X$ run until time $T$ and 0 otherwise becomes indistinguishable from the uniform measure on such markings at the threshold $T=1/2T_{\mathrm {cov}}(\mathbf {Z}_n^d)$. As a consequence of our methods, we show that the total variation mixing time of the random walk on the lamplighter graph $\mathbf {Z}_2\wr \mathbf {Z}_n^d$, $d\geq3$, has a cutoff with threshold $1/2T_{\mathrm {cov}}(\mathbf {Z}_n^d)$. We give a general criterion under which both of these results hold; other examples for which this applies include bounded degree expander families, the intersection of an infinite supercritical percolation cluster with an increasing family of balls, the hypercube and the Caley graph of the symmetric group generated by transpositions. The proof also yields precise asymptotics for the decay of correlation in the uncovered set.

math.PR↗

Universality for SLE(4)

We resolve a conjecture of Sheffield that $\SLE(4)$, a conformally invariant random curve, is the universal limit of the chordal zero-height contours of random surfaces with isotropic, uniformly convex potentials. Specifically, we study the \emph{Ginzburg-Landau $\nabla ϕ$ interface model} or \emph{anharmonic crystal} on $D_n = D \cap \tfrac{1}{n} \Z^2$ for $D \subseteq \C$ a bounded, simply connected Jordan domain with smooth boundary. This is the massless field with Hamiltonian $\CH(h) = \sum_{x \sim y} \CV(h(x) - h(y))$ with $\CV$ symmetric and uniformly convex and $h(x) = ϕ(x)$ for $x \in \partial D_n$, $ϕ\colon \partial D_n \to \R$ a given function. We show that the macroscopic chordal contours of $h$ are asymptotically described by $\SLE(4)$ for appropriately chosen $ϕ$.

math.PR↗

Thick points of the Gaussian free field

Let $U\subseteq\mathbf{C}$ be a bounded domain with smooth boundary and let $F$ be an instance of the continuum Gaussian free field on $U$ with respect to the Dirichlet inner product $\int_U\nabla f(x)\cdot \nabla g(x)\,dx$. The set $T(a;U)$ of $a$-thick points of $F$ consists of those $z\in U$ such that the average of $F$ on a disk of radius $r$ centered at $z$ has growth $\sqrt{a/π}\log\frac{1}{r}$ as $r\to 0$. We show that for each $0\leq a\leq2$ the Hausdorff dimension of $T(a;U)$ is almost surely $2-a$, that $ν_{2-a}(T(a;U))=\infty$ when $0 2$. Furthermore, we prove that $T(a;U)$ is invariant under conformal transformations in an appropriate sense. The notion of a thick point is connected to the Liouville quantum gravity measure with parameter $γ$ given formally by $Γ(dz)=e^{\sqrt{2π}γF(z)}\,dz$ considered by Duplantier and Sheffield.

math.PR↗

Fluctuations for the Ginzburg-Landau $\nabla ϕ$ Interface Model on a Bounded Domain

We study the massless field on $D_n = D \cap \tfrac{1}{n} \Z^2$, where $D \subseteq \R^2$ is a bounded domain with smooth boundary, with Hamiltonian $\CH(h) = \sum_{x \sim y} \CV(h(x) - h(y))$. The interaction $\CV$ is assumed to be symmetric and uniformly convex. This is a general model for a $(2+1)$-dimensional effective interface where $h$ represents the height. We take our boundary conditions to be a continuous perturbation of a macroscopic tilt: $h(x) = n x \cdot u + f(x)$ for $x \in \partial D_n$, $u \in \R^2$, and $f \colon \R^2 \to \R$ continuous. We prove that the fluctuations of linear functionals of $h(x)$ about the tilt converge in the limit to a Gaussian free field on $D$, the standard Gaussian with respect to the weighted Dirichlet inner product $(f,g)_\nabla^β= \int_D \sum_i β_i \partial_i f_i \partial_i g_i$ for some explicit $β= β(u)$. In a subsequent article, we will employ the tools developed here to resolve a conjecture of Sheffield that the zero contour lines of $h$ are asymptotically described by $SLE(4)$, a conformally invariant random curve.

math.PR↗

Quasi-stationary Random Overlap Structures and the Continuous Cascades

A random overlap structure (ROSt) is a measure on pairs (X,Q) where X is a locally finite sequence in the real line with a maximum and Q a positive semidefinite matrix of overlaps intrinsic to the particles X. Such a measure is said to be quasi-stationary provided that the joint law of the gaps of X and overlaps Q is stable under a stochastic evolution driven by a Gaussian sequence with covariance Q. Aizenman et al. have shown that quasi-stationary ROSts serve as an important computational tool in the study of the Sherrington-Kirkpatrick (SK) spin-glass model from the perspective of cavity dynamics and the related ROSt variational principle for its free energy. In this framework, the Parisi solution is reflected in the ansatz that the overlap matrix exhibit a certain hierarchical structure. Aizenman et al. have posed the question of whether the ansatz could be explained by showing that the only ROSts that are quasi-stationary in a robust sense are given by a special class of hierarchical ROSts known as both the Ruelle Probability Cascades as well the GREM. Arguin and Aizenman have given an affirmative answer in the special case that the set of values S_Q taken on by the entries of Q is finite. We prove that this result holds even when |S_Q| is infinite provided that Q satisfies the technical condition that the closure of S_Q has no limit points from below. This is relevant to the understanding of the ground states of the SK model, as they satisfy |S_Q| = infinity.

math.PR↗