Emergent Planarity in two-dimensional Ising Models with finite-range Interactions
arXiv:1801.04960 · doi:10.1007/s00222-018-00851-4
Abstract
The known Pfaffian structure of the boundary spin correlations, and more generally order-disorder correlation functions, is given a new explanation through simple topological considerations within the model's random current representation. This perspective is then employed in the proof that the Pfaffian structure of boundary correlations emerges asymptotically at criticality in Ising models on with finite-range interactions. The analysis is enabled by new results on the stochastic geometry of the corresponding random currents. The proven statement establishes an aspect of universality, seen here in the emergence of fermionic structures in two dimensions beyond the solvable cases.
arXiv comment59 pages, 19 figures
References in corpus (8)
- The Random-Cluster Model
- A new proof of the sharpness of the phase transition for Bernoulli percolation and the Ising model
- Random Currents and Continuity of Ising Model's Spontaneous Magnetization
- Revisiting the combinatorics of the 2D Ising model
- A note on Ising random currents, Ising-FK, loop-soups and the Gaussian free field
- The scaling limit of the energy correlations in non integrable Ising models
- The planar Ising model and total positivity
- Kac-Ward formula and its extension to order-disorder correlators through a graph zeta function
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