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Publication date: Jan 23, 2025
Superelasticity, being a reversible nonlinear strain response to stress stimuli beyond the linear elastic regime, is always associated with phase transformations in its host materials, mostly metals or polymers. Theoretical rationale indicates that inorganic materials with covalent/ionic bonding normally have large energy barriers for reversible structural transitions and thus host less opportunity to achieve superelasticity. Here, we demonstrate a directional tensile superelasticity in ceramic crystal GeSe through an unconventional reversible shuffle twinning mechanism instead of martensitic phase transition. We observed, with in-situ mechanical transmission electron microscopy, an evolution in stress‒strain curve from the linear elastic behavior to a nonlinear superelastic plateau, and confirmed that such superelasticity appears simultaneously together with the generation of stripy-shaped twin domains along orientation. Theoretical calculations revealed that the shuffle twinning process from “Z-shaped” to “anti-Z-shaped” bond-configuration leads to the release of elastic potential energy, being responsible for the emergence of tensile superelasticity therein. Note that such a highly-directional superelasticity prefers to emerge at angles near the zigzag direction owing to the anisotropic Young’s modulus and Poisson’s ratio in GeSe, and has never been reported in superelastic materials. Our observation provides a novel strategy to exploit tensile superelasticity and nonlinear mechanics for advanced mechanical and flexible electronics.
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File name | Size | Description |
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Additional In-situ TEM videos of GeSe superelasticity.zip
MD5md5:871cdcad431994852f3412e42acd1621
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2.2 GiB | The videos recording the evolution of twin domains in GeSe via in-situ TEM |
GeSe-videos-caption.txt
MD5md5:f036b65793f9d93bda6f0e17d767e00e
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1.0 KiB | Captions of "Additional In-situ TEM videos of GeSe superelasticity" |
2025.17 (version v1) [This version] | Jan 23, 2025 | DOI10.24435/materialscloud:98-53 |