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Absence of critical thickness for polar skyrmions with breaking the Kittel’s law

The period of polar domain (d) in ferroics was commonly believed to scale with corresponding film thicknesses (h), following the classical Kittel’s law of d ∝ [Formula: see text] . Here, we have not only observed that this relationship fails in the case of polar skyrmions, where the period shrinks n...

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Detalles Bibliográficos
Autores principales: Gong, Feng-Hui, Tang, Yun-Long, Wang, Yu-Jia, Chen, Yu-Ting, Wu, Bo, Yang, Li-Xin, Zhu, Yin-Lian, Ma, Xiu-Liang
Formato: Online Artículo Texto
Lenguaje:English
Publicado: Nature Publishing Group UK 2023
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10250330/
https://www.ncbi.nlm.nih.gov/pubmed/37291226
http://dx.doi.org/10.1038/s41467-023-39169-y
Descripción
Sumario:The period of polar domain (d) in ferroics was commonly believed to scale with corresponding film thicknesses (h), following the classical Kittel’s law of d ∝ [Formula: see text] . Here, we have not only observed that this relationship fails in the case of polar skyrmions, where the period shrinks nearly to a constant value, or even experiences a slight increase, but also discovered that skyrmions have further persisted in [(PbTiO(3))(2)/(SrTiO(3))(2)](10) ultrathin superlattices. Both experimental and theoretical results indicate that the skyrmion periods (d) and PbTiO(3) layer thicknesses in superlattice (h) obey the hyperbolic function of d = Ah + [Formula: see text] other than previous believed, simple square root law. Phase-field analysis indicates that the relationship originates from the different energy competitions of the superlattices with PbTiO(3) layer thicknesses. This work exemplified the critical size problems faced by nanoscale ferroelectric device designing in the post-Moore era.