Microelectromechanical systems (MEMS) have recently found strong interest in academia and industry. They result from the integration of mechanical elements, sensors, actuators, and electronics onto a silicon substrate. [ 1 ] The miniaturization of integrated systems offers the advantage of high effi ciency at low fabrication costs and novel functionalities. This emerging technology has led to a strong demand for micro-and nanometerscaled actuators. [ 2 ] Liquid-crystalline elastomers (LCEs) [3][4][5][6] are a class of functional materials that have been used for the fabrication of actuators for many years. Consisting of weakly crosslinked polymer chains that are covalently linked to stiff, shape-anisotropic molecules (mesogens), they combine the ability of self-organization from liquid crystals with the entropy elasticity of elastomers. Depending on the ambient conditions, these mesogens can either be in an unordered state (isotropic phase) or self-organized into ordered liquidcrystalline phases. In the isotropic phase, the polymer chains can adopt the entropically favored random-coil conformation. On the other hand, if the mesogens align into a liquid-crystalline phase, the polymer chains have to respond to the resulting anisotropic environment and adapt an anisotropic conformation. A phase transition between the liquid-crystalline and isotropic phases thus allows switching of the polymer backbone between these two conformations. This conformational change comes along with a macroscopic change of the sample's dimensions, [ 7 ] which enables the utilization of LCEs as materials for actuator applications. [ 6 , 8 , 9 ] Every stimulus that leads to a phase transition in the liquid-crystalline material (heat, UV light, presence of a solvent) can be used to trigger the actuation process. As a result of the reversibility of liquid-crystalline phase transitions, the change in shape is reversible as well. It has to be mentioned that these shape-changing effects can only be