Abstract
We consider low temperature limits of Gibbs states of the ferromagnetic nearest-neighbour Ising Hamiltonian in the positive orthant of the lattice ℤ d ,d=1, 2,..., under a negative boundary condition and a small positive external fieldh that decreases linearly with the temperatureT. It is shown that positive and negative spins are separated by a “staircase-shaped” random boundary. Its explicit distribution is computed in the case that the ratio α=h/T exceeds some positiveα0. Forα <α0, our results do not rule out infinite negative areas.
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