Optomechanics combines optical and mechanical degrees of freedom to enable new applications and to attain new parameter regimes. The simplest optomechanical system consists of only a single optical and a single mechanical mode. Such a system can serve as a quantum memory where an optical excitation is stored in the long lived mechanical excitation [1]. Conversely, the optomechanical interaction allows one to prepare quantum mechanical states of motion opening the door to the experimental exploration of quantum mechanics in massive system [2].Over recent years optomechanical systems have gained in complexity, exploring multiple optical and/or mechanical modes. In those systems, mechanical degrees can mediate between different optical modes allowing to convert quantum excitations between the optical and the microwave domains [3]. On the other hand, the optical field can also couple dissimilar mechanical modes, which is useful for synchronizing the mechanical vibrations [4]. Now, Piergentili et al exploit a multimodal optomechanical system to increase the optomechanical coupling strength [5].The paradigmatic case of an optomechanical system consists of a Fabry-Pérot cavity where one of the cavity mirrors is free to move around its equilibrium position. The mechanical motion couples dispersively to the cavity, that is, the cavity frequency is shifted by a displacement of the mechanical elements, leading to the optomechanical couplingwhere ω c and L are the cavity frequency and its length, respectively. Piergentili et alʼs work [5] is based on a very successful variation of the paradigmatic Fabry-Pérot optomechanical cavity, where the end mirrors are fixed and a membrane is placed inside the cavity [6]. Even though the cavity length is constant, the optical path length depends on the position of the membrane along the cavity axis. This leads to an optomechanical coupling, where θ m is the mode-overlap between the mechanical mode of the membrane and the optical cavity mode, which depends on the membrane refractive index and position. Thus, the optomechanical coupling increases for smaller cavities since the electromagnetic field is more concentrated and, consequently, microscopic cavities achieve the highest coupling strengths [7]. However, a small cavity comes with a faster cavity decay k µ L 1 because the round trip time of photons in the cavity is proportional to its length.An alternative strategy is to enhance the interaction by increasing the number of mechanical elements [8]. This allows one, for instance, to achieve a strong optomechanical interaction with ensembles of atoms, where the optomechanical interaction of each atom is rather small but the interaction of a collective mode of the ensemble is increased by a factor of N 1/2 . A single atom is a weak scatterer and does not modify the cavity field. In contrast, a single membrane strongly modifies the cavity field and interference of the scattered fields can lead to an even stronger scaling µ N 3 2 with the number of membranes [8], specifically in transmissiv...