Fig. 2: Local structures of the crystals. | Nature Communications

Fig. 2: Local structures of the crystals.

From: Deciphering the atomistic mechanism underlying highly tunable piezoelectric properties in perovskite ferroelectrics via transition metal doping

Fig. 2

AC The high-angle annular dark-field (HAADF) images of the pristine, Fe-doped, and Mn-doped KTN crystals, obtained along the [001]C direction at room temperature, respectively. The small and large bright points represent the A-site and B-site ions, respectively. Mappings of the polar vectors are marked by yellow arrows in (AC). The atomic displacements are presented as vectors pointing from the center of a B-site cation to the center of its four nearest neighboring A-site cations. These atomic displacements represent the magnitudes and directions of the polar vectors for each unit-cell column. The x, y, and z directions correspond to the [100]C, [010]C, and [001]C crystallographic directions, respectively. The statistical scatterplots of the absolute value of the angle between the polar vector and the x-axis are shown in (DF) for pristine, Fe-doped, and Mn-doped samples, respectively. GI Distributions of shear strain exy and JL phase of piezoresponse force microscopy (PFM) images on the (001)C faces of the pristine, Fe-doped, and Mn-doped samples, respectively. The white color in the exy distribution maps indicates the zero exy strain regions. The exx, eyy, and Rtot distributions are shown in Fig. S4.

Back to article page