light the whole structure is described as a metamaterial [1][2][3]. A monolithic membrane traversed by a parallel array of cylindrical nanochannels represents such a metamaterial, see illustration in Fig. 1. The advent of tailorable porosity at the nanoscale and thus of an adjustable "meta-atomic" structure offers new opportunities to tailor the optical anisotropy of such metamaterials. Effective optical properties, not achievable by base materials, are possible [2-8], specifically adjustable birefringence. This is of particular relevance for important polarisation management components, such as waveplates and compensators, that play an essential part in modern optical communication systems [9].A versatile route to fine-tune optics of porous materials is filling the pore space with a liquid crystal (LC) [10,11]. In the bulk case LCs play a dominant role for the manipulation of optical anisotropy [12]. By embedding LCs in nanoporous media the self-assembly and self-healing mechanisms can be used to design a new soft-hard metamaterial. The LC adds optical functionality, whereas the arXiv:1911.10052v1 [cond-mat.soft]