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. 2007 Dec 12;104(51):20204–20209. doi: 10.1073/pnas.0709316104

Fig. 4.

Fig. 4.

Phase-field modeling of polarization switching mechanism in BiFeO3. (a) Variation of nucleation voltage as a function of gamma. (b) Spatial distribution of nucleation potential along the line A–B–C shown by the dotted line in Inset (domain structure under short-circuit boundary conditions). The polarization directions are indicated. (c and d) Histograms of positive and negative nucleation and coercive biases, respectively.