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Application of an electric field to favour ferroelectric domains whose polarization aligns with the field, leaving a net remanent polarization. In a ceramic the crystal grains remain differently oriented; domain switching does not align their crystallographic axes.

For a conventional initially random, untextured piezoceramic, orientational averaging suppresses the macroscopic linear response. Electrical poling of ferroelectric domains is the usual way to generate a lasting net response. Under that conventional preparation assumption, a ferroelectric constituent is the expected route.

However, the word polycrystalline alone does not logically require ferroelectricity. A deliberately textured aggregate of nonswitchable piezoelectric grains can have a nonzero effective tensor if their orientations and polar directions do not cancel. Ferroelectricity means electrically switchable spontaneous polarization, whereas piezoelectricity means linear stress–charge coupling. Thus the unconditional statement that every polycrystalline piezoelectric must be ferroelectric is too strong.

In piezoresponse force microscopy, a conducting atomic force microscopy tip contacts a sample with a counter-electrode. Apply $V(t)=V_{\mathrm{dc}}+V_{\mathrm{ac}}\cos \omega t$. The converse piezoelectric effect produces an oscillatory displacement, approximately $u_{\omega }=d_{\mathrm{eff}}{V}_{\mathrm{ac}}$. Contact with the moving surface bends the cantilever, and a lock-in amplifier records the displacement amplitude and phase relative to the drive.

For opposite out-of-plane ferroelectric domains, the effective piezoelectric coefficient changes sign. Their vertical response therefore differs by approximately $180^{\circ }$ in phase. Equivalent antiparallel domains can have similar amplitudes, while cancellation or reduced response near a wall can produce an amplitude minimum. Phase identifies the relative response sign; an uncalibrated detector phase is not an absolute polarization direction.

Use a small drive below the switching threshold while imaging, a stable contact force and a well-characterized contact resonance. Electrostatic forces, contact stiffness and surface charging can also create signals at the drive frequency; observing contrast alone is insufficient evidence for polarization switching.^[ref]