This paper is studying the critical regime of the planar random-cluster model on with cluster-weight . More precisely, we prove which are uniform in their boundary conditions and depend only on their extremal lengths. They imply in particular that any fractal boundary is touched by macroscopic clusters, uniformly in its roughness or the configuration on the boundary. Additionally, they imply that . We also obtain a number of properties of so-called arm-events: (two arms in the half-plane, three arms in the half-plane and five arms in the bulk), and properties (even when arms are not alternating between primal and dual), and the fact that the . These results were previously known only for Bernoulli percolation ( ) and the FK-Ising model ( ). Finally, we prove new bounds on the one, two and four-arm exponents for , as well as the one-arm exponent in the half-plane. These improve the previously known bounds, even for Bernoulli percolation.
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http://dx.doi.org/10.1007/s00440-021-01060-6 | DOI Listing |
Probab Theory Relat Fields
June 2021
ETHZ, Zürich, Switzerland.
This paper is studying the critical regime of the planar random-cluster model on with cluster-weight . More precisely, we prove which are uniform in their boundary conditions and depend only on their extremal lengths. They imply in particular that any fractal boundary is touched by macroscopic clusters, uniformly in its roughness or the configuration on the boundary.
View Article and Find Full Text PDFAnn Henri Poincare
June 2020
Munich Center for Quantum Science and Technology, 80799 Munich, Germany.
The ground-states of the spin- antiferromagnetic chain with a projection-based interaction and the spin-1/2 XXZ-chain at anisotropy parameter share a common loop representation in terms of a two-dimensional functional integral which is similar to the classical planar -state Potts model at . The multifaceted relation is used here to directly relate the distinct forms of translation symmetry breaking which are manifested in the ground-states of these two models: dimerization for at all , and Néel order for at . The results presented include: (i) a translation to the above quantum spin systems of the results which were recently proven by Duminil-Copin-Li-Manolescu for a broad class of two-dimensional random-cluster models, and (ii) a short proof of the symmetry breaking in a manner similar to the recent structural proof by Ray-Spinka of the discontinuity of the phase transition for .
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