Lifetime scaling for stripe metastable states under Z2-symmetric perturbations in the 2d Ising model
Prove that, for the two-dimensional Ising model initialized in a stripe metastable state and subjected to perturbations that preserve the Ising \mathbb{Z}_2 symmetry, the lifetime t_* scales as exp(c·ℓ²) in the stripe width ℓ. Establish this scaling rigorously by analyzing the resonant rectangle-flipping channel alone, in the absence of false-vacuum decay, starting from genuine metastable states where each stripe corresponds to a true ground state of the symmetric Hamiltonian.
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Furthermore, if we require that the perturbation preserves the Ising \mathbb{Z}2 symmetry, there is no longer a false vacuum decay as in Section \ref{sec:falsevacuum}, so we expect (but did not prove) that t* = \exp{\Omega(\ell2)} coming from the latter channel alone, so long as one starts from the genuine metastable state where each stripe corresponds to a "true ground state" of the symmetric Hamiltonian.