Fig. 1: Comparison of the various properties for pristine, Fe-doped, and Mn-doped KTN crystals. | Nature Communications

Fig. 1: Comparison of the various properties for pristine, Fe-doped, and Mn-doped KTN crystals.

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

Fig. 1

AC Dielectric constant εr as a function of temperature and frequency, DF strain–electric field (S–E) loops at 1 Hz, GI polarization–electric field (P–E) loops, current–electric field (J–E) loops at 1 Hz, J dielectric losses tan δ at 100 kHz, K internal bias fields, Eint, extracted from PE loops, and L lateral-mode mechanical quality factors, Qm, for pristine, Fe-doped, and Mn-doped KTN crystals, respectively. The orthorhombic–tetragonal phase transition temperatures of 50 °C are marked in (AC), and the insets show the corresponding low-temperature dielectric properties in the range of −150 to 0 °C. The arrow in (C) inset indicates a frequency dependence of dielectric maxima at the rhombohedral-to-orthorhombic phase transition, showing a typical relaxor behavior. The insets in (DF) are the photos giving the results of quasi-static d33 tests. In the SE, PE, and Qm measurements, the samples poled along the [001]C crystallographic direction were used. The magnitude of Eint is determined by Eint = (E+ + E)/2, where E+ and E are the intersections of polarization loop with positive and negative electric field axis.

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