Diamond is a material of choice in the pursuit of integrated quantum photonic technologies. So far, the majority of photonic devices fabricated from diamond, are made from (100)-oriented crystals. In this work, we demonstrate a methodology for the fabrication of optically-active membranes from (111)-oriented diamond. We use a liftoff technique to generate membranes, followed by chemical vapour deposition of diamond in the presence of silicon to generate homogenous silicon vacancy colour centers with emission properties that are superior to those in (100)-oriented diamond. We further use the diamond membranes to fabricate high quality microring resonators with quality factors exceeding ~ 3000. Supported by finite difference time domain calculations, we discuss the advantages of (111) oriented structures as building blocks for quantum nanophotonic devices.Diamond is an attractive platform for studies of light-matter interaction at the nanoscale[1-7]. In the past decade, defects in diamond, also known as color centers, have emerged as attractive candidates for scalable solid state quantum photonic architectures [1,6]. While earlier works were focused predominantly on nitrogen vacancy (NV) centres [8,9], recent effort is devoted to group IV defects [10][11][12][13][14][15], (e.g. the silicon vacancy (SiV)) due to their narrowband emission and a better resilience to electromagnetic fluctuations.Integration of these color centres with photonic resonators is an important challenge for several reasons. First, it enables enhancement of the photon emission flux from the single color centres (for instance by using diamond pillars [16]). Second, it provides the means to interconnect potential quantum nodes in a large network, where the emitters are coupled to individual cavities and interconnected with a waveguide [17,18]. Last, if the photonic resonator is carefully designed with coupled directional emission, one can achieve high cavity cooperativity and realise advanced quantum phenomena such as single photon switch with a solid state system [19]. However, despite the remarkable progress in nanofabrication of diamond cavities [8,20], all photonic resonators to date were fabricated from (100)-oriented diamond, primarily because this is the most common orientation provided by commercial suppliers and the difficulty in engineering and polishing (111) oriented crystals [21]. This, however, limits the potential coupling strength of many color centers to cavities since most centers studied to date have dipoles oriented along the <111> direction, and the dipole overlap with the cavity field is therefore not optimal in cavities fabricated from (100)-oriented diamond. Conversely, in (111)-oriented diamond, the overlap is optimal, and superior Purcell enhancement is expected.In the current work, we fabricated large area (111) diamond membranes that exhibit bright SiV luminescence. Consequently, these membranes were utilized to engineer high quality diamond microring resonators with quality factors of ~ 3000. Our work launches a new ...