In studies using piezoresponse force microscopy, we observe a nonzero lateral piezoresponse at 180°d omain walls in out-of-plane polarized, c-axis-oriented tetragonal ferroelectric Pb͑Zr 0.2 Ti 0.8 ͒O 3 epitaxial thin films. We attribute these observations to a shear strain effect linked to the sign change of the d 33 piezoelectric coefficient through the domain wall, in agreement with theoretical predictions. We show that in monoclinically distorted tetragonal BiFeO 3 films, this effect is superimposed on the lateral piezoresponse due to actual in-plane polarization and has to be taken into account in order to correctly interpret the ferroelectric domain configuration. © 2009 American Institute of Physics. ͓doi:10.1063/1.3226654͔ Ferroelectric materials, characterized by their reversible spontaneous electric polarization, show great potential for multifunctional applications ranging from nonvolatile memories 1,2 to nanoscale sensors and actuators. 3 Controlling the structure and stability of ferroelectric domains in these materials is a key requirement for device implementation. In particular, the dynamics of domain walls, the interfaces separating regions with differently oriented ferroelectric polarization in the films, can significantly affect performance. 4 Understanding domain wall behavior at the nanoscopic scales of current and future devices, however, requires techniques with the requisite nanoscale resolution.One such technique is piezoresponse force microscopy ͑PFM͒, 5 in which a metallic atomic force microscope ͑AFM͒ tip is used to apply an alternating voltage across the ferroelectric material, resulting in a local mechanical response at the film surface due to the inverse piezoelectric effect. This piezoelectric response can be detected from the induced displacement of the AFM cantilever, recorded by the position of a laser beam reflected onto a quadrant-split photodetector. The vertical deflection and angular torsion of the tip are referred to as vertical and lateral PFM, respectively. The response phase provides information on the polarization, while its amplitude is related to the polarization magnitude. 6 Depending on the piezoelectric coefficient tensor d ij , linked to the crystal symmetry, a combination of these two measurements allows access to both out-of-plane and in-plane components of polarization. Although quantitative measurements of piezoelectric coefficients via PFM are challenging, the technique has provided valuable information about the behavior of domain walls and switching dynamics both in thin films 7,8 and in device structures. [9][10][11] In this context, understanding the origins of the PFM signal observed at ferroelectric domain walls is an important issue.Considering only piezoelectric effects, in a c-axis-oriented tetragonal ferroelectric film with an electric field applied along the polarization axis, the piezoelectric response is determined by the d 33 coefficient, leading to a purely vertical PFM signal. However, in such films, a nonzero lateral PFM response has been ...