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arxiv: 2508.18241 · v1 · pith:JOK4AY6Hnew · submitted 2025-08-25 · ❄️ cond-mat.mtrl-sci

Atomistic Structure of Transient Switching States in Ferroelectric AlScN

classification ❄️ cond-mat.mtrl-sci
keywords switchingdomainferroelectricstemalscnbehaviordynamicsexperimental
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We resolve the microscopic mechanism of polarization switching in wurtzite ferroelectric AlScN by integrating advanced thin-film fabrication, ferroelectric switching dynamics characterizations, high-resolution scanning transmission electron microscopy (STEM), and large-scale molecular dynamics simulations enabled by a deep neural network-based interatomic potential. Contrary to earlier interpretations proposing a transient nonpolar intermediate phase, we demonstrate that the broad transitional regions previously observed in STEM images are projection artifacts resulting from the intrinsic three-dimensional zigzag morphology of 180$^\circ$ domain walls, which are a characteristic form of inversion domain boundary. This is further confirmed by STEM imaging of strategically prepared, partially switched Al$_{0.75}$Sc$_{0.25}$N thin films. Our simulations reveal that switching proceeds through collective, column-by-column atomic displacements, directly explaining the emergence of zigzag-shaped domain walls, and is consistent with the nucleation-limited switching behavior observed in experimental switching dynamic measurements. Furthermore, we show that increasing Sc content systematically lowers domain wall energy and associated nucleation barrier, thereby reducing the switching field in agreement with experimental trends. These findings establish a direct connection between local domain wall structure, switching kinetics, and macroscopic ferroelectric behavior.

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  1. Domain-Wall Mediated Polarization Switching in Ferroelectric AlScN: Strain Relief and Field-Dependent Dynamics

    cond-mat.mtrl-sci 2025-08 unverdicted novelty 5.0

    Domain walls mediate strain relief and enable field-dependent polarization switching in AlScN, following domain-wall propagation at low fields and nonlinear nucleation at high fields.