Abstract. We study the collective behavior of inclusions inducing local anisotropic curvatures in a flexible fluid membrane. The N -body interaction energy for general anisotropic inclusions is calculated explicitly, including multi-body interactions. Long-range attractive interactions between inclusions are found to be sufficiently strong to induce aggregation. Monte Carlo simulations show a transition from compact clusters to aggregation on lines or circles. These results might be relevant to proteins in biological membranes or colloidal particles bound to surfactant membranes.PACS. 87.15. The interplay between structural features and N -body interactions is a general physical problem arising in many different contexts, e.g., crystals structure [1], magnetic atom clusters [2,3], colloids in charged fluids [4], polyelectrolyte condensation [5,6], and protein aggregation in biological membranes [7]. N -body interactions can sometimes yield spectacular effects: non-pairwise summability of charge fluctuation forces can dramatically affect the stability of polyelectrolyte bundles [5]; three-body elastic interactions may induce aggregation of membrane inclusions, although two-body elastic interactions are repulsive [7]. In a system able to kinetically achieve equilibrium, the clusters formed are usually compact, however certain interactions may favor tenuous clusters. For instance, a recent N -body study has shown that above a critical strength of three-body interactions, the state of minimum energy is one in which all the particles are on a line [8]. It has also been observed recently that membrane mediated interactions can induce one-dimensional ring-like aggregates of colloidal particles bound to fluid vesicle membranes [9].Manifolds embedded in a correlated elastic medium can impose boundary conditions, or modify the elastic constants. This usually gives rise to mean-field forces, which are due to the elastic deformation of the medium, and to Casimir forces, which are due to the modification of its thermal fluctuations. Such interactions are generally non pairwise additive [10]. The elastic interactions between defects in solids [11] or in liquid crystals [12] are well known examples of mean-field forces. Casimir forces exist between manifolds embedded in correlated fluids, such as liquid crystals and superfluids [13,14,10], or critical mixtures [15]. Another interesting example is the interaction between inclusions in flexible membranes [16]: it has been shown that cone shaped membrane inclusions experience both long range attractive Casimir interactions and repulsive elastic interactions falling of as R −4 with separation R [17].In this Rapid Note, following Netz [18], we give exact results concerning the long range multi-body interactions among membrane inclusions that break the bilayer's updown symmetry. However, rather than supposing that the inclusions simply induce a local spontaneous curvature, we assume that the inclusions set a preferred curvature tensor [17,19]. This model is more realistic: the "pre...