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Marked GUE-corners process in doubly periodic dimer models

Tomas Berggren, Nedialko Bradinoff

Abstract

We study a family of periodically weighted Aztec diamond dimer models near their turning points. We establish that, asymptotically, as $N\rightarrow\infty$, their fluctuations there, scaled by $\sqrt{N}$, are described by a marked GUE-corners process. This limiting point process is constructed by assigning a Bernoulli mark independently to each particle in a realization of the GUE-corners process. The Bernoulli parameters associated with the random marks reflect the periodicity of the model in the limit. To prove this result we use a double-contour integral representation of the inverse Kasteleyn matrix on a higher-genus Riemann surface, which is well-suited for asymptotic analysis.

Marked GUE-corners process in doubly periodic dimer models

Abstract

We study a family of periodically weighted Aztec diamond dimer models near their turning points. We establish that, asymptotically, as , their fluctuations there, scaled by , are described by a marked GUE-corners process. This limiting point process is constructed by assigning a Bernoulli mark independently to each particle in a realization of the GUE-corners process. The Bernoulli parameters associated with the random marks reflect the periodicity of the model in the limit. To prove this result we use a double-contour integral representation of the inverse Kasteleyn matrix on a higher-genus Riemann surface, which is well-suited for asymptotic analysis.

Paper Structure

This paper contains 21 sections, 25 theorems, 130 equations, 7 figures.

Key Result

Theorem 1.1

Let $K_{\operatorname{Int}}$ be the correlation kernel of $(u_{s}^t)_{1\leq s\leq t\leq 2\ell N}$ and suppose $\nu:\mathbb{Z}_{>0}\times \{0,1\} \rightarrow \mathbb{R}$ is given by where $\alpha_{\ell-t}$ and $\beta_{\ell-t}$ are the edge weights of the model (see Figure fig:Aztec_diamond_graph_4 and later eqn:edge_weights). Let the gauge function $g:\{0,1,\ldots, 2\ell N\}^2\rightarrow \mathbb{R

Figures (7)

  • Figure 1: The Aztec diamond graph of size 4 on the left and the fundamental domain of the $2\times 4$ periodically weighted Aztec diamond dimer model on the right. North, East, South, and West edges are colored blue, orange, red, and green respectively.
  • Figure 2: The two interlacing particle systems near the turning point, in grey and black, defined from South (yellow) and West (red) edges from a random outcome of the Aztec diamond; The picture is rotated so that the first particle is at the bottom instead of to the right. Dimers in the picture are illustrated as dominoes.
  • Figure 3: Left: The particles defined from the dimers visualized in red and cyan. The color depends on the parity of the coordinates of the particle. Right: A dimer cover of the Aztec diamond of size $4$. The particles form an interlacing particle system.
  • Figure 4: The Riemann surface $\mathcal{R}$ represented as two copies of the complex plane. The cuts (dashed) are located along the negative part of the real lines. The compact ovals $A_k$, $k=1,\dots,\ell-1$ (solid) are located along the negative part of the real lines, and the non-compact oval $A_0$ (solid) are located along the positive part of the real lines. The gray areas are connected via the cuts, and so are the white areas. In this illustration, the curve $\tilde{\Gamma}_s$ (blue) is a simple loop, while $\tilde{\Gamma}_l$ (red) is the union of two simple loops.
  • Figure 5: Contours of integration for the integral representation of the GUE-corners process; $\gamma_s'$ is drawn in blue and $\gamma_{\ell'}$ is drawn in red when $\mu_1<\mu_2$ and in a dashed grey line for $\mu_1> \mu_2$.
  • ...and 2 more figures

Theorems & Definitions (56)

  • Theorem 1.1: Theorem \ref{['thm:limit_correlation_function']}
  • Theorem 1.2: Corollary \ref{['cor:week_converence']}
  • Corollary 1.3: Corollary \ref{['cor:thinned']}
  • Lemma 2.1
  • proof
  • Lemma 2.2: JN06
  • proof
  • Lemma 2.3: Ber21
  • Theorem 2.4
  • proof
  • ...and 46 more