TY - JOUR
T1 - Non-constant Ground Configurations in the Disordered Ferromagnet
AU - Bassan, Michal
AU - Gilboa, Shoni
AU - Peled, Ron
N1 - Publisher Copyright:
© The Author(s), under exclusive licence to Springer-Verlag GmbH Germany, part of Springer Nature 2025.
PY - 2025/10/3
Y1 - 2025/10/3
N2 - The disordered ferromagnet is a disordered version of the ferromagnetic Ising model in which the coupling constants are non-negative quenched random. A ground configuration is an infinite-volume configuration whose energy cannot be reduced by finite modifications. It is a long-standing challenge to ascertain whether the disordered ferromagnet on the ZD lattice admits non-constant ground configurations. We answer this affirmatively in dimensions D≥4, when the coupling constants are sampled independently from a sufficiently concentrated distribution. The obtained ground configurations are further shown to be translation-covariant with respect to ZD-1 translations of the disorder. Our result is proved by showing that the finite-volume interface formed by Dobrushin boundary conditions is localized, and converges to an infinite-volume interface. This may be expressed in purely combinatorial terms, as a result on the fluctuations of certain minimal cutsets in the lattice ZD endowed with independent edge capacities.
AB - The disordered ferromagnet is a disordered version of the ferromagnetic Ising model in which the coupling constants are non-negative quenched random. A ground configuration is an infinite-volume configuration whose energy cannot be reduced by finite modifications. It is a long-standing challenge to ascertain whether the disordered ferromagnet on the ZD lattice admits non-constant ground configurations. We answer this affirmatively in dimensions D≥4, when the coupling constants are sampled independently from a sufficiently concentrated distribution. The obtained ground configurations are further shown to be translation-covariant with respect to ZD-1 translations of the disorder. Our result is proved by showing that the finite-volume interface formed by Dobrushin boundary conditions is localized, and converges to an infinite-volume interface. This may be expressed in purely combinatorial terms, as a result on the fluctuations of certain minimal cutsets in the lattice ZD endowed with independent edge capacities.
UR - https://www.scopus.com/pages/publications/105018206177
U2 - 10.1007/s00220-025-05395-2
DO - 10.1007/s00220-025-05395-2
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AN - SCOPUS:105018206177
SN - 0010-3616
VL - 406
JO - Communications in Mathematical Physics
JF - Communications in Mathematical Physics
IS - 11
M1 - 266
ER -