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Page 10 of 12       Zhang et al. Microstructures 2023;3:2023010  https://dx.doi.org/10.20517/microstructures.2022.39

               surface, the electric field converges towards the probe tip, as the inset indicates. The Cu ions migrate to the
               probe and decrease the Schottky barrier between the probe and the sample. The effective electric field
               directly acting on the CIPS phase is enough to switch the domain, and the yellow domain is switched to the
               black domain. On the contrary, when a voltage of +6 V is applied, the direction of the electric field diverges
               from the probe, and the Cu ions are driven away from the tip, and the effective electric field acting on the
               CIPS phase therefore cannot switch domain. As a result, all domains did not change significantly, and the
               overall piezoelectric response decreased. To confirm ion mobility in CIPS-IPS, we characterized the
               macroscopically manifested I-V curves, and the results are shown in Figure 4F. In the upward polarization
               region, we can find that the forward current gradually increases as the rate of the applied bias cycle
               decreases. Likewise, in the downward polarization region, the forward current is also large at lower voltage
               sweep speeds. Nevertheless, with the increase of scanning speed, the whole forward current decreases until
               zero, while the reverse current gradually increases and tends to be stable. All suggest that Cu ion migration
               dominates the current feature, which is consistent with our previous studies on current regulation in pure
               CIPS . These results favorably confirm that Cu ions mediate the switching of ferroelectric domains.
                   [16]

               CONCLUSIONS
               In conclusion, we accurately characterized the Young’s modulus of the CIPS-IPS two phases for the first
               time by various experimental methods (nanoindentation method and atomic force contact resonance
               method) in this study, and the Young’s modulus of the CIPS phase was 27.42 ± 0.05 GPa, slightly less than
               that of the IPS phase, which was 27.51 ± 0.04 GPa. In addition, we calculated the elastic matrices of the two
               phases of CIPS-IPS using the first-principles method, and deduced their respective Young’s modulus, all of
               which are in good agreement with our experimental values. Finally, we also discover the asymmetry of
               domain switching and propose an ion-mediated nonreciprocal domain switching model, which strongly
               explains this interesting phenomenon. Our work provides a reliable experimental reference for the follow-
               up study of the elastic properties of CIPS-IPS and the phase field simulation for regulating the domain
               structure.

               DECLARATIONS
               Authors’ contributions
               AFM characterization, writing original draft: Zhang X
               Review & editing, supervision: Jiang X
               Raman characterization: Du G
               DFT calculation: Ren Q
               EDS characterization: Zhu W
               Sample synthesis: Kang J, Deng J
               Guidance for experiment and data analysis: Lun Y, Wang T, Bai B, Yu Z
               Conceptualization, review, supervision: Hong J, Wang X, Chen Y


               Availability of data and materials
               The list of elemental atomic percentages of different CIPS flakes obtained from EDS, single-point CRF
               measurement results of CIPS-IPS and HOPG by CR-AFM, CR-AFM method, A: frequency and friction
               histogram and original PFM data are provided in Supplementary Information.


               Financial support and sponsorship
               The work at Beijing Institute of Technology is supported by National Natural Science Foundation of China
               with Grant Nos. 12172047, 11604011, 92163101, 12202056, National Key Research and Development
               Program of China (2019YFA0307900), the Beijing Natural Science Foundation (Z190011), and Beijing
               Institute of Technology Research Fund Program for Young Scholars.
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