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Switching Time in Ferroelectric BaTiO3 and Its Dependence on Crystal Thickness

Merz, Walter J.·1956·Journal of Applied Physics

Abstract

The switching time ts and the switching current imax have been measured as a function of applied field E and of the size of the sample. It has been observed that the ``activation field'' α for the nucleation of new domains is inversely proportional to the thickness of the sample. This behavior can be explained by assuming a surface layer. The thickness of this layer has been calculated to be of the order of 10−4 cm. The same way we can explain the thickness dependence of the 60-cycle coercive field strength. Furthermore, it has been found that the switching time depends to a first approximation linearly on the thickness of the sample if the field E is kept constant. This can be explained by assuming a domain wall motion primarily in the forward direction or by assuming a nucleation mechanism. The maximum velocity of the domain growth was found to be of the order of the velocity of sound. The switching time does not depend on electrode area.

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Metadata

Authors
Merz, W. J.
Venue
Journal of Applied Physics
Published
1956-08-01
Volume
27
Issue
8
Pages
938-943
ISSN
  • 0021-8979 (ISSN-L)
  • 1089-7550
OpenAlex
W2036941130
Cited by
495
References
0
FWCI
14.43
Type
journal article
Language
en
Open access
closed

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CoChat. (2026). Citation check: Switching Time in Ferroelectric BaTiO3 and Its Dependence on Crystal Thickness. https://app.cochat.ai/papers/10.1063/1.1722518
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Merz, W. J. (1956). Switching Time in Ferroelectric BaTiO3 and Its Dependence on Crystal Thickness. Journal of Applied Physics. https://doi.org/10.1063/1.1722518

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Semantic Scholar’s data is described in: Kinney, R., et al. (2023). The Semantic Scholar Open Data Platform. arXiv:2301.10140.