The Doob transform and the tree behind the forest, with application to near-critical dimers - Archive ouverte HAL
Pré-Publication, Document De Travail Année : 2024

The Doob transform and the tree behind the forest, with application to near-critical dimers

Résumé

The Doob transform technique enables the study of a killed random walk (KRW) via a random walk (RW) with transition probabilities tilted by a discrete massive harmonic function. The main contribution of this paper is to transfer this powerful technique to statistical mechanics by relating two models, namely random rooted spanning forests (RSF) and random spanning trees (RST), and provide applications. More precisely, our first main theorem explicitly relates models on the level of partition functions, and probability measures, in the case of finite and infinite graphs. Then, in the planar case, we also rely on the dimer model: we introduce a killed and a drifted dimer model, extending to this general framework the models introduced in [Chh12, dT20]. Using Temperley's bijection between RST and dimers, this allows us to relate RSF to dimers and thus extend partially this bijection to RSF. As immediate applications, we give a short and transparent proof of Kenyon's result stating that the spectral curve of RSF is a Harnack curve, and provide a general setting to relate discrete massive holomorphic and harmonic functions. The other important application consists in proving universality of the convergence of the near-critical loop-erased RW, RST and dimer models by extending the results of [CW21, Chh12, HSB22] from the square lattice to any isoradial graphs: we introduce a loop-erased RW, RST and dimer model on isoradial discretizations of any simply connected domain and prove convergence in the massive scaling limit towards continuous objects described by a massive version of SLE2.
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Dates et versions

hal-04417909 , version 1 (25-01-2024)

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Lucas Rey. The Doob transform and the tree behind the forest, with application to near-critical dimers. 2024. ⟨hal-04417909⟩
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