light of wavelengths commensurate to their periodicity and, depending on their arrangement and composition, they form photonic structures of different complexity, ranging from 1D gratings (Bragg grating) up to 3D photonic crystals. In all these cases, light-matter interaction leads to characteristic optical features, such as reflection and transmission profiles of diffractive gratings and, even more interestingly, the propagation inhibition of certain frequencies (photonic band gap) in photonic crystals. Surprisingly, nature presents numerous examples of how optical properties can be affected by nanoscale structuration. In fact, many living organisms adopt structural coloration, [1] a nanometric arrangement of dielectric geometric units on their skin or shell, to create vivid and bright structural colors. This way they adapt to the surrounding environment, send warning messages, or mislead their natural enemies through camouflage. [2] Mimic nature, and in particular actual reconfigurable mechanisms, [3] is fundamental also in man-made photonic applications to control the optical response of devices or materials. Current strategies include the use of the electrooptic effect, [4] temperature sensitivity, [5] and carrier injection. [6] Another method relies on the birefringent behavior of liquid crystals (LCs), [7] which can be infiltrated in photonic structures allowing to control the refractive index through temperature, [8] electric, [9] or magnetic [10] fields. Materials with structural color can be effectively-but invasively and slowly-tuned by deforming them, for instance by applying mechanical pressure or stress. [11] This is the only proposed tuning method over the optical response that acts on the unit cell variation instead of relying on refractive index control. Here we wish to explore a different route to achieve tuning and switching of photonic materials, using the light itself as a means to control the mechanical state of a periodic material. By creating a structured material out of photoresponsive polymer, we show that it is possible to induce mechanical deformation-and hence a huge change in the optical response of the material-by simply shining light on it. De facto, this constitutes a nonlinear optical effect, with sub-millisecond time response, using mechanical deformation as an intermediate step. The deformation, and hence the nonlinear response, takes place only in the illuminated region and therefore can be precisely local. The photoresponsive polymers that we use are light sensitive liquid crystal networks (LCN), [12] or elastomers, which have the ability to strongly deform in a reproducible way. [13] It has been demonstrated that LCN can be Materials whose optical response is determined by their structure are of much interest both for their fundamental properties and applications. Examples range from simple gratings to photonic crystals. Obtaining control over the optical properties is of crucial importance in this context, and it is often attempted by electro-optical effect or by using m...