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Topological ferroelectric chirality

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arxiv 2406.19728 v1 pith:R3ONYVMM submitted 2024-06-28 cond-mat.mtrl-sci cond-mat.mes-hallphysics.optics

classification cond-mat.mtrl-scicond-mat.mes-hallphysics.optics
keywords chiralitytopologicalapplicationschiraldevelopmentsferroelectricferroelectricsmaterials
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Chirality, an inherent property of most objects of the universe, is a dynamic research topic in material science, physics, chemistry, and biology. The fundamental appeal of this extensive study is supported by the technological quest to manufacture materials with configurable chiralities for emerging applications ranging from optoelectronics and photonics to pharmaceutics and medicine. Recent advances put forth ferroelectrics as a host of chiral topological states in the form of Bloch domain walls, skyrmions, merons, and Hopfions, offering thus a unique ground for making chirality switchable and tunable. Here we review current developments, milestones achieved, and future routes of chiral ferroelectric materials. We focus on insights into the topological origin of the chirality in the nanostructured ferroelectrics, bringing new controllable functionalities. We pay special attention to novel developments enabling tunability and manipulating the chiroptical response and enantioselectivity, leading to new applications in nano-optoelectronics, plasmonics, pharmaceutics, and bio-medical industries.

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Cited by 2 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Morphology of Polarization States in Strained Ferroelectric Films

    cond-mat.mtrl-sci 2025-09 conditional novelty 6.0 of 10

    A single-mode variational ansatz yields phase diagrams of vortex, helix, wave, and uniform polarization states in strained PbTiO3 films as functions of temperature, strain, and thickness.

  2. Twist, splay, and uniform domains in ferroelectric nematic liquid crystals

    cond-mat.soft 2025-02 conditional novelty 6.0 of 10

    In ferroelectric nematic cells with apolar anchoring, domain size is set by a competition between depolarization electrostatics and domain wall elasticity, with wall energy scaling linearly with cell thickness.

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