Reveals that every low-energy switching path must cross a mesoscopic wall shell, indicating its fundamental role in dynamics.
We study dynamical crossing paths in a two-dimensional interacting block-spin strip under local single-spin-flip dynamics. Previous work established that the minimal strip-crossing energy is of order L_y*K*sqrt(J), that every minimizer contains a mesoscopic wall of total central-band volume L_y*sqrt(J), and that near-optimal walls are rigid up to a controlled number of kinks. The present paper addresses the corresponding dynamical question: whether every near-optimal minus-to-plus switching path must traverse a mesoscopic wall shell. We prove that any path whose maximal energy remains within A*K*sqrt(J) of the optimal strip-crossing barrier must contain an intermediate configuration whose rowwise central-band structure forms a wall shell of mesoscopic width and controlled rigidity. Thus the static wall is not merely an optimizer of a boundary-value problem: it is dynamically unavoidable along low-barrier switching paths. The paper should be read as a two-dimensional dynamical bridge preprint rather than as a full bottleneck theorem. Related earlier works by S. Pan are available at DOI: 10.5281/zenodo.19673404, DOI: 10.5281/zenodo.19689210, DOI: 10.5281/zenodo.19690441, DOI: 10.5281/zenodo.19693231, DOI: 10.5281/zenodo.19696148, and DOI: 10.5281/zenodo.19697539.
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S. Pan (2026) studied this question.
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