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February 21, 20260 citationsOpen Access

The multinomial dimer model

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RKRichard KenyonCWCatherine Wolfram

Key Points

  • The aim is to analyze the multinomial dimer model's behavior on periodic bipartite graphs under scaling limits.
  • Studied N-dimer covers on bipartite graphs in R^d.
  • Proved a large deviation principle with an explicit surface tension.
  • Analyzed the convergence of critical gauge functions in the scaling limit.
  • Computed explicit limit shapes for specific 2D and 3D examples.
  • Random configurations concentrate around a unique limit shape.
  • Limit shapes correspond to solutions of an associated Euler-Lagrange equation.
  • First successful computation of limit shapes in 3D statistical mechanics models.

Abstract

An N-dimer cover of a graph is a collection of edges (with multiplicity) such that each vertex is contained in exactly N edges in the collection. The multinomial dimer model is a natural probability measure on N-dimer covers. We study the behavior of these measures on periodic bipartite graphs in R d , in the scaling limit as the multiplicity N and then the size of the graph go to infinity. In this iterated limit, we prove a large deviation principle, where the rate function is the integral of an explicit surface tension, and show that random configurations concentrate on a limit shape which is the unique solution to an associated Euler-Lagrange equation. We further show that the associated critical gauge functions, which exist in the N → ∞ limit on each finite graph, converge in the scaling limit to a limiting gauge function which solves a dual Euler-Lagrange equation. We use our techniques to compute explicit limit shapes in some two and three dimensional examples, such as the Aztec diamond and “Aztec cuboid”. These 3d examples are the first stat mech models in dimensions d ≥ 3 where limit shapes can be computed explicitly.

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Cite This Study

Kenyon et al. (2025) studied this question.

synapsesocial.com/papers/69994cdf873532290d021bc6https://doi.org/10.3929/ethz-c-000793862
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