After calculations of various domain‐switching current transients under the pulse from electrical circuit parameters, the field dependence of domain‐switching speeds is accurately estimated over five orders of magnitude in a wide temperature range of 5.4–280 K from the height of domain‐switching current in Pb(Zr 0.4 Ti 0.6 )O 3 thin films. These estimations are extended following Merz's equation [W. J. Merz, Phys. Rev. 1954 , 95 , 690] and an ultimate domain‐switching current density of 1.4 × 10 8 A cm −1 is extracted at the highest field of 0.20 MV cm −1 . From classical domain‐nucleation models with thermal fluctuations, an ultimate (asymptotic high‐field) nucleation time of 0.47 ps is derived when the domain sideways motion is kink‐nucleation‐rate limited.
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Jiang et al. (2011) studied this question.
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